Maksimov and Kolovsky, Equation (3)

Percentage Accurate: 73.3% → 99.8%
Time: 4.5s
Alternatives: 12
Speedup: 0.4×

Specification

?
\[\begin{array}{l} \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}} \end{array} \end{array} \]
(FPCore (J K U)
 :precision binary64
 (let* ((t_0 (cos (/ K 2.0))))
   (* (* (* -2.0 J) t_0) (sqrt (+ 1.0 (pow (/ U (* (* 2.0 J) t_0)) 2.0))))))
double code(double J, double K, double U) {
	double t_0 = cos((K / 2.0));
	return ((-2.0 * J) * t_0) * sqrt((1.0 + pow((U / ((2.0 * J) * t_0)), 2.0)));
}
module fmin_fmax_functions
    implicit none
    private
    public fmax
    public fmin

    interface fmax
        module procedure fmax88
        module procedure fmax44
        module procedure fmax84
        module procedure fmax48
    end interface
    interface fmin
        module procedure fmin88
        module procedure fmin44
        module procedure fmin84
        module procedure fmin48
    end interface
contains
    real(8) function fmax88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(4) function fmax44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(8) function fmax84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmax48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
    end function
    real(8) function fmin88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(4) function fmin44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(8) function fmin84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmin48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
    end function
end module

real(8) function code(j, k, u)
use fmin_fmax_functions
    real(8), intent (in) :: j
    real(8), intent (in) :: k
    real(8), intent (in) :: u
    real(8) :: t_0
    t_0 = cos((k / 2.0d0))
    code = (((-2.0d0) * j) * t_0) * sqrt((1.0d0 + ((u / ((2.0d0 * j) * t_0)) ** 2.0d0)))
end function
public static double code(double J, double K, double U) {
	double t_0 = Math.cos((K / 2.0));
	return ((-2.0 * J) * t_0) * Math.sqrt((1.0 + Math.pow((U / ((2.0 * J) * t_0)), 2.0)));
}
def code(J, K, U):
	t_0 = math.cos((K / 2.0))
	return ((-2.0 * J) * t_0) * math.sqrt((1.0 + math.pow((U / ((2.0 * J) * t_0)), 2.0)))
function code(J, K, U)
	t_0 = cos(Float64(K / 2.0))
	return Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))))
end
function tmp = code(J, K, U)
	t_0 = cos((K / 2.0));
	tmp = ((-2.0 * J) * t_0) * sqrt((1.0 + ((U / ((2.0 * J) * t_0)) ^ 2.0)));
end
code[J_, K_, U_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \cos \left(\frac{K}{2}\right)\\
\left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}
\end{array}
\end{array}

Local Percentage Accuracy vs ?

The average percentage accuracy by input value. Horizontal axis shows value of an input variable; the variable is choosen in the title. Vertical axis is accuracy; higher is better. Red represent the original program, while blue represents Herbie's suggestion. These can be toggled with buttons below the plot. The line is an average while dots represent individual samples.

Accuracy vs Speed?

Herbie found 12 alternatives:

AlternativeAccuracySpeedup
The accuracy (vertical axis) and speed (horizontal axis) of each alternatives. Up and to the right is better. The red square shows the initial program, and each blue circle shows an alternative.The line shows the best available speed-accuracy tradeoffs.

Initial Program: 73.3% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}} \end{array} \end{array} \]
(FPCore (J K U)
 :precision binary64
 (let* ((t_0 (cos (/ K 2.0))))
   (* (* (* -2.0 J) t_0) (sqrt (+ 1.0 (pow (/ U (* (* 2.0 J) t_0)) 2.0))))))
double code(double J, double K, double U) {
	double t_0 = cos((K / 2.0));
	return ((-2.0 * J) * t_0) * sqrt((1.0 + pow((U / ((2.0 * J) * t_0)), 2.0)));
}
module fmin_fmax_functions
    implicit none
    private
    public fmax
    public fmin

    interface fmax
        module procedure fmax88
        module procedure fmax44
        module procedure fmax84
        module procedure fmax48
    end interface
    interface fmin
        module procedure fmin88
        module procedure fmin44
        module procedure fmin84
        module procedure fmin48
    end interface
contains
    real(8) function fmax88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(4) function fmax44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(8) function fmax84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmax48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
    end function
    real(8) function fmin88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(4) function fmin44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(8) function fmin84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmin48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
    end function
end module

real(8) function code(j, k, u)
use fmin_fmax_functions
    real(8), intent (in) :: j
    real(8), intent (in) :: k
    real(8), intent (in) :: u
    real(8) :: t_0
    t_0 = cos((k / 2.0d0))
    code = (((-2.0d0) * j) * t_0) * sqrt((1.0d0 + ((u / ((2.0d0 * j) * t_0)) ** 2.0d0)))
end function
public static double code(double J, double K, double U) {
	double t_0 = Math.cos((K / 2.0));
	return ((-2.0 * J) * t_0) * Math.sqrt((1.0 + Math.pow((U / ((2.0 * J) * t_0)), 2.0)));
}
def code(J, K, U):
	t_0 = math.cos((K / 2.0))
	return ((-2.0 * J) * t_0) * math.sqrt((1.0 + math.pow((U / ((2.0 * J) * t_0)), 2.0)))
function code(J, K, U)
	t_0 = cos(Float64(K / 2.0))
	return Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))))
end
function tmp = code(J, K, U)
	t_0 = cos((K / 2.0));
	tmp = ((-2.0 * J) * t_0) * sqrt((1.0 + ((U / ((2.0 * J) * t_0)) ^ 2.0)));
end
code[J_, K_, U_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \cos \left(\frac{K}{2}\right)\\
\left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}
\end{array}
\end{array}

Alternative 1: 99.8% accurate, 0.3× speedup?

\[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(K \cdot 0.5\right)\\ t_1 := \cos \left(\frac{K}{2}\right)\\ t_2 := \left(\left(-2 \cdot J\right) \cdot t\_1\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_1}\right)}^{2}}\\ \mathbf{if}\;t\_2 \leq -\infty:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{elif}\;t\_2 \leq 10^{+307}:\\ \;\;\;\;\left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
U_m = (fabs.f64 U)
(FPCore (J K U_m)
 :precision binary64
 (let* ((t_0 (cos (* K 0.5)))
        (t_1 (cos (/ K 2.0)))
        (t_2
         (*
          (* (* -2.0 J) t_1)
          (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_1)) 2.0))))))
   (if (<= t_2 (- INFINITY))
     (* -2.0 (* U_m 0.5))
     (if (<= t_2 1e+307)
       (*
        (* (* -2.0 J) t_0)
        (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_0)) 2.0))))
       (* -2.0 (* -0.5 U_m))))))
U_m = fabs(U);
double code(double J, double K, double U_m) {
	double t_0 = cos((K * 0.5));
	double t_1 = cos((K / 2.0));
	double t_2 = ((-2.0 * J) * t_1) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_1)), 2.0)));
	double tmp;
	if (t_2 <= -((double) INFINITY)) {
		tmp = -2.0 * (U_m * 0.5);
	} else if (t_2 <= 1e+307) {
		tmp = ((-2.0 * J) * t_0) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_0)), 2.0)));
	} else {
		tmp = -2.0 * (-0.5 * U_m);
	}
	return tmp;
}
U_m = Math.abs(U);
public static double code(double J, double K, double U_m) {
	double t_0 = Math.cos((K * 0.5));
	double t_1 = Math.cos((K / 2.0));
	double t_2 = ((-2.0 * J) * t_1) * Math.sqrt((1.0 + Math.pow((U_m / ((2.0 * J) * t_1)), 2.0)));
	double tmp;
	if (t_2 <= -Double.POSITIVE_INFINITY) {
		tmp = -2.0 * (U_m * 0.5);
	} else if (t_2 <= 1e+307) {
		tmp = ((-2.0 * J) * t_0) * Math.sqrt((1.0 + Math.pow((U_m / ((2.0 * J) * t_0)), 2.0)));
	} else {
		tmp = -2.0 * (-0.5 * U_m);
	}
	return tmp;
}
U_m = math.fabs(U)
def code(J, K, U_m):
	t_0 = math.cos((K * 0.5))
	t_1 = math.cos((K / 2.0))
	t_2 = ((-2.0 * J) * t_1) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_1)), 2.0)))
	tmp = 0
	if t_2 <= -math.inf:
		tmp = -2.0 * (U_m * 0.5)
	elif t_2 <= 1e+307:
		tmp = ((-2.0 * J) * t_0) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_0)), 2.0)))
	else:
		tmp = -2.0 * (-0.5 * U_m)
	return tmp
U_m = abs(U)
function code(J, K, U_m)
	t_0 = cos(Float64(K * 0.5))
	t_1 = cos(Float64(K / 2.0))
	t_2 = Float64(Float64(Float64(-2.0 * J) * t_1) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_1)) ^ 2.0))))
	tmp = 0.0
	if (t_2 <= Float64(-Inf))
		tmp = Float64(-2.0 * Float64(U_m * 0.5));
	elseif (t_2 <= 1e+307)
		tmp = Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))));
	else
		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
	end
	return tmp
end
U_m = abs(U);
function tmp_2 = code(J, K, U_m)
	t_0 = cos((K * 0.5));
	t_1 = cos((K / 2.0));
	t_2 = ((-2.0 * J) * t_1) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_1)) ^ 2.0)));
	tmp = 0.0;
	if (t_2 <= -Inf)
		tmp = -2.0 * (U_m * 0.5);
	elseif (t_2 <= 1e+307)
		tmp = ((-2.0 * J) * t_0) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_0)) ^ 2.0)));
	else
		tmp = -2.0 * (-0.5 * U_m);
	end
	tmp_2 = tmp;
end
U_m = N[Abs[U], $MachinePrecision]
code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K * 0.5), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$1), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$1), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$2, (-Infinity)], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$2, 1e+307], N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]]
\begin{array}{l}
U_m = \left|U\right|

\\
\begin{array}{l}
t_0 := \cos \left(K \cdot 0.5\right)\\
t_1 := \cos \left(\frac{K}{2}\right)\\
t_2 := \left(\left(-2 \cdot J\right) \cdot t\_1\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_1}\right)}^{2}}\\
\mathbf{if}\;t\_2 \leq -\infty:\\
\;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\

\mathbf{elif}\;t\_2 \leq 10^{+307}:\\
\;\;\;\;\left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\

\mathbf{else}:\\
\;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\


\end{array}
\end{array}
Derivation
  1. Split input into 3 regimes
  2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0

    1. Initial program 73.3%

      \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
    2. Taylor expanded in J around 0

      \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
    3. Step-by-step derivation
      1. lower-*.f64N/A

        \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
      2. lower-*.f64N/A

        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
      3. lower-cos.f64N/A

        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
      4. lower-*.f64N/A

        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
      5. lower-sqrt.f64N/A

        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
      6. lower-*.f64N/A

        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
      7. lower-/.f64N/A

        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
      8. lower-pow.f64N/A

        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
      9. lower-pow.f64N/A

        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
      10. lower-cos.f64N/A

        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
      11. lower-*.f6414.8

        \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
    4. Applied rewrites14.8%

      \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
    5. Taylor expanded in U around 0

      \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
    6. Step-by-step derivation
      1. lower-*.f64N/A

        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
      2. lower-*.f64N/A

        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
      3. lower-cos.f64N/A

        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
      4. lower-*.f64N/A

        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
      5. lower-sqrt.f64N/A

        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
      6. lower-/.f64N/A

        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
      7. lower-pow.f64N/A

        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
      8. lower-cos.f64N/A

        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
      9. lower-*.f6425.6

        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
    7. Applied rewrites25.6%

      \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
    8. Taylor expanded in K around 0

      \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
    9. Step-by-step derivation
      1. Applied rewrites26.4%

        \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

      if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < 9.99999999999999986e306

      1. Initial program 73.3%

        \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
      2. Step-by-step derivation
        1. lift-/.f64N/A

          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \color{blue}{\left(\frac{K}{2}\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
        2. mult-flipN/A

          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \color{blue}{\left(K \cdot \frac{1}{2}\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
        3. metadata-evalN/A

          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(K \cdot \color{blue}{\frac{1}{2}}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
        4. lower-*.f6473.3

          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \color{blue}{\left(K \cdot 0.5\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
      3. Applied rewrites73.3%

        \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \color{blue}{\left(K \cdot 0.5\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
      4. Step-by-step derivation
        1. lift-/.f64N/A

          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(K \cdot \frac{1}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \color{blue}{\left(\frac{K}{2}\right)}}\right)}^{2}} \]
        2. mult-flipN/A

          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(K \cdot \frac{1}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \color{blue}{\left(K \cdot \frac{1}{2}\right)}}\right)}^{2}} \]
        3. metadata-evalN/A

          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(K \cdot \frac{1}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(K \cdot \color{blue}{\frac{1}{2}}\right)}\right)}^{2}} \]
        4. lower-*.f6473.3

          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(K \cdot 0.5\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \color{blue}{\left(K \cdot 0.5\right)}}\right)}^{2}} \]
      5. Applied rewrites73.3%

        \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(K \cdot 0.5\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \color{blue}{\left(K \cdot 0.5\right)}}\right)}^{2}} \]

      if 9.99999999999999986e306 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

      1. Initial program 73.3%

        \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
      2. Taylor expanded in J around 0

        \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
      3. Step-by-step derivation
        1. lower-*.f64N/A

          \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
        2. lower-*.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
        3. lower-cos.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
        4. lower-*.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        5. lower-sqrt.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        6. lower-*.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        7. lower-/.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        8. lower-pow.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        9. lower-pow.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        10. lower-cos.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        11. lower-*.f6414.8

          \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
      4. Applied rewrites14.8%

        \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
      5. Taylor expanded in K around 0

        \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
      6. Step-by-step derivation
        1. lower-sqrt.f64N/A

          \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
        2. lower-*.f64N/A

          \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
        3. lower-pow.f6414.9

          \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
      7. Applied rewrites14.9%

        \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
      8. Taylor expanded in U around -inf

        \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
      9. Step-by-step derivation
        1. lower-*.f6426.5

          \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
      10. Applied rewrites26.5%

        \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
    10. Recombined 3 regimes into one program.
    11. Add Preprocessing

    Alternative 2: 98.2% accurate, 0.3× speedup?

    \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(K \cdot -0.5\right)\\ t_1 := \cos \left(\frac{K}{2}\right)\\ t_2 := \left(\left(-2 \cdot J\right) \cdot t\_1\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_1}\right)}^{2}}\\ \mathbf{if}\;t\_2 \leq -\infty:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{elif}\;t\_2 \leq 10^{+307}:\\ \;\;\;\;\left(\left(t\_0 \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U\_m}{\left(J + J\right) \cdot t\_0}\right)\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
    U_m = (fabs.f64 U)
    (FPCore (J K U_m)
     :precision binary64
     (let* ((t_0 (cos (* K -0.5)))
            (t_1 (cos (/ K 2.0)))
            (t_2
             (*
              (* (* -2.0 J) t_1)
              (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_1)) 2.0))))))
       (if (<= t_2 (- INFINITY))
         (* -2.0 (* U_m 0.5))
         (if (<= t_2 1e+307)
           (* (* (* t_0 -2.0) J) (cosh (asinh (/ U_m (* (+ J J) t_0)))))
           (* -2.0 (* -0.5 U_m))))))
    U_m = fabs(U);
    double code(double J, double K, double U_m) {
    	double t_0 = cos((K * -0.5));
    	double t_1 = cos((K / 2.0));
    	double t_2 = ((-2.0 * J) * t_1) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_1)), 2.0)));
    	double tmp;
    	if (t_2 <= -((double) INFINITY)) {
    		tmp = -2.0 * (U_m * 0.5);
    	} else if (t_2 <= 1e+307) {
    		tmp = ((t_0 * -2.0) * J) * cosh(asinh((U_m / ((J + J) * t_0))));
    	} else {
    		tmp = -2.0 * (-0.5 * U_m);
    	}
    	return tmp;
    }
    
    U_m = math.fabs(U)
    def code(J, K, U_m):
    	t_0 = math.cos((K * -0.5))
    	t_1 = math.cos((K / 2.0))
    	t_2 = ((-2.0 * J) * t_1) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_1)), 2.0)))
    	tmp = 0
    	if t_2 <= -math.inf:
    		tmp = -2.0 * (U_m * 0.5)
    	elif t_2 <= 1e+307:
    		tmp = ((t_0 * -2.0) * J) * math.cosh(math.asinh((U_m / ((J + J) * t_0))))
    	else:
    		tmp = -2.0 * (-0.5 * U_m)
    	return tmp
    
    U_m = abs(U)
    function code(J, K, U_m)
    	t_0 = cos(Float64(K * -0.5))
    	t_1 = cos(Float64(K / 2.0))
    	t_2 = Float64(Float64(Float64(-2.0 * J) * t_1) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_1)) ^ 2.0))))
    	tmp = 0.0
    	if (t_2 <= Float64(-Inf))
    		tmp = Float64(-2.0 * Float64(U_m * 0.5));
    	elseif (t_2 <= 1e+307)
    		tmp = Float64(Float64(Float64(t_0 * -2.0) * J) * cosh(asinh(Float64(U_m / Float64(Float64(J + J) * t_0)))));
    	else
    		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
    	end
    	return tmp
    end
    
    U_m = abs(U);
    function tmp_2 = code(J, K, U_m)
    	t_0 = cos((K * -0.5));
    	t_1 = cos((K / 2.0));
    	t_2 = ((-2.0 * J) * t_1) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_1)) ^ 2.0)));
    	tmp = 0.0;
    	if (t_2 <= -Inf)
    		tmp = -2.0 * (U_m * 0.5);
    	elseif (t_2 <= 1e+307)
    		tmp = ((t_0 * -2.0) * J) * cosh(asinh((U_m / ((J + J) * t_0))));
    	else
    		tmp = -2.0 * (-0.5 * U_m);
    	end
    	tmp_2 = tmp;
    end
    
    U_m = N[Abs[U], $MachinePrecision]
    code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K * -0.5), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$1), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$1), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$2, (-Infinity)], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$2, 1e+307], N[(N[(N[(t$95$0 * -2.0), $MachinePrecision] * J), $MachinePrecision] * N[Cosh[N[ArcSinh[N[(U$95$m / N[(N[(J + J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision], N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]]
    
    \begin{array}{l}
    U_m = \left|U\right|
    
    \\
    \begin{array}{l}
    t_0 := \cos \left(K \cdot -0.5\right)\\
    t_1 := \cos \left(\frac{K}{2}\right)\\
    t_2 := \left(\left(-2 \cdot J\right) \cdot t\_1\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_1}\right)}^{2}}\\
    \mathbf{if}\;t\_2 \leq -\infty:\\
    \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\
    
    \mathbf{elif}\;t\_2 \leq 10^{+307}:\\
    \;\;\;\;\left(\left(t\_0 \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U\_m}{\left(J + J\right) \cdot t\_0}\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 3 regimes
    2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0

      1. Initial program 73.3%

        \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
      2. Taylor expanded in J around 0

        \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
      3. Step-by-step derivation
        1. lower-*.f64N/A

          \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
        2. lower-*.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
        3. lower-cos.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
        4. lower-*.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        5. lower-sqrt.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        6. lower-*.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        7. lower-/.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        8. lower-pow.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        9. lower-pow.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        10. lower-cos.f64N/A

          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
        11. lower-*.f6414.8

          \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
      4. Applied rewrites14.8%

        \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
      5. Taylor expanded in U around 0

        \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
      6. Step-by-step derivation
        1. lower-*.f64N/A

          \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
        2. lower-*.f64N/A

          \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
        3. lower-cos.f64N/A

          \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
        4. lower-*.f64N/A

          \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
        5. lower-sqrt.f64N/A

          \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
        6. lower-/.f64N/A

          \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
        7. lower-pow.f64N/A

          \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
        8. lower-cos.f64N/A

          \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
        9. lower-*.f6425.6

          \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
      7. Applied rewrites25.6%

        \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
      8. Taylor expanded in K around 0

        \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
      9. Step-by-step derivation
        1. Applied rewrites26.4%

          \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

        if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < 9.99999999999999986e306

        1. Initial program 73.3%

          \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
        2. Step-by-step derivation
          1. lift-*.f64N/A

            \[\leadsto \color{blue}{\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          2. *-commutativeN/A

            \[\leadsto \color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot \left(-2 \cdot J\right)\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          3. lift-*.f64N/A

            \[\leadsto \left(\cos \left(\frac{K}{2}\right) \cdot \color{blue}{\left(-2 \cdot J\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          4. associate-*r*N/A

            \[\leadsto \color{blue}{\left(\left(\cos \left(\frac{K}{2}\right) \cdot -2\right) \cdot J\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          5. lower-*.f64N/A

            \[\leadsto \color{blue}{\left(\left(\cos \left(\frac{K}{2}\right) \cdot -2\right) \cdot J\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          6. lower-*.f6473.4

            \[\leadsto \left(\color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot -2\right)} \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          7. lift-cos.f64N/A

            \[\leadsto \left(\left(\color{blue}{\cos \left(\frac{K}{2}\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          8. cos-neg-revN/A

            \[\leadsto \left(\left(\color{blue}{\cos \left(\mathsf{neg}\left(\frac{K}{2}\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          9. lower-cos.f64N/A

            \[\leadsto \left(\left(\color{blue}{\cos \left(\mathsf{neg}\left(\frac{K}{2}\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          10. lift-/.f64N/A

            \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(\color{blue}{\frac{K}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          11. mult-flipN/A

            \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(\color{blue}{K \cdot \frac{1}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          12. metadata-evalN/A

            \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(K \cdot \color{blue}{\frac{1}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          13. distribute-rgt-neg-inN/A

            \[\leadsto \left(\left(\cos \color{blue}{\left(K \cdot \left(\mathsf{neg}\left(\frac{1}{2}\right)\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          14. metadata-evalN/A

            \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{\frac{-1}{2}}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          15. metadata-evalN/A

            \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{\frac{1}{-2}}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          16. lower-*.f64N/A

            \[\leadsto \left(\left(\cos \color{blue}{\left(K \cdot \frac{1}{-2}\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          17. metadata-eval73.4

            \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{-0.5}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          18. lift-sqrt.f64N/A

            \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \color{blue}{\sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
          19. lift-+.f64N/A

            \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{\color{blue}{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
        3. Applied rewrites84.8%

          \[\leadsto \color{blue}{\left(\left(\cos \left(K \cdot -0.5\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U}{\left(J + J\right) \cdot \cos \left(K \cdot -0.5\right)}\right)} \]

        if 9.99999999999999986e306 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

        1. Initial program 73.3%

          \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
        2. Taylor expanded in J around 0

          \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
        3. Step-by-step derivation
          1. lower-*.f64N/A

            \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
          2. lower-*.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
          3. lower-cos.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
          4. lower-*.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          5. lower-sqrt.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          6. lower-*.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          7. lower-/.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          8. lower-pow.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          9. lower-pow.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          10. lower-cos.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          11. lower-*.f6414.8

            \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
        4. Applied rewrites14.8%

          \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
        5. Taylor expanded in K around 0

          \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
        6. Step-by-step derivation
          1. lower-sqrt.f64N/A

            \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
          2. lower-*.f64N/A

            \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
          3. lower-pow.f6414.9

            \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
        7. Applied rewrites14.9%

          \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
        8. Taylor expanded in U around -inf

          \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
        9. Step-by-step derivation
          1. lower-*.f6426.5

            \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
        10. Applied rewrites26.5%

          \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
      10. Recombined 3 regimes into one program.
      11. Add Preprocessing

      Alternative 3: 98.2% accurate, 0.3× speedup?

      \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\ t_2 := \cos \left(K \cdot -0.5\right)\\ \mathbf{if}\;t\_1 \leq -\infty:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{elif}\;t\_1 \leq 10^{+307}:\\ \;\;\;\;\left(\cosh \sinh^{-1} \left(\frac{U\_m}{\left(J + J\right) \cdot t\_2}\right) \cdot \left(J \cdot -2\right)\right) \cdot t\_2\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
      U_m = (fabs.f64 U)
      (FPCore (J K U_m)
       :precision binary64
       (let* ((t_0 (cos (/ K 2.0)))
              (t_1
               (*
                (* (* -2.0 J) t_0)
                (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_0)) 2.0)))))
              (t_2 (cos (* K -0.5))))
         (if (<= t_1 (- INFINITY))
           (* -2.0 (* U_m 0.5))
           (if (<= t_1 1e+307)
             (* (* (cosh (asinh (/ U_m (* (+ J J) t_2)))) (* J -2.0)) t_2)
             (* -2.0 (* -0.5 U_m))))))
      U_m = fabs(U);
      double code(double J, double K, double U_m) {
      	double t_0 = cos((K / 2.0));
      	double t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_0)), 2.0)));
      	double t_2 = cos((K * -0.5));
      	double tmp;
      	if (t_1 <= -((double) INFINITY)) {
      		tmp = -2.0 * (U_m * 0.5);
      	} else if (t_1 <= 1e+307) {
      		tmp = (cosh(asinh((U_m / ((J + J) * t_2)))) * (J * -2.0)) * t_2;
      	} else {
      		tmp = -2.0 * (-0.5 * U_m);
      	}
      	return tmp;
      }
      
      U_m = math.fabs(U)
      def code(J, K, U_m):
      	t_0 = math.cos((K / 2.0))
      	t_1 = ((-2.0 * J) * t_0) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_0)), 2.0)))
      	t_2 = math.cos((K * -0.5))
      	tmp = 0
      	if t_1 <= -math.inf:
      		tmp = -2.0 * (U_m * 0.5)
      	elif t_1 <= 1e+307:
      		tmp = (math.cosh(math.asinh((U_m / ((J + J) * t_2)))) * (J * -2.0)) * t_2
      	else:
      		tmp = -2.0 * (-0.5 * U_m)
      	return tmp
      
      U_m = abs(U)
      function code(J, K, U_m)
      	t_0 = cos(Float64(K / 2.0))
      	t_1 = Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))))
      	t_2 = cos(Float64(K * -0.5))
      	tmp = 0.0
      	if (t_1 <= Float64(-Inf))
      		tmp = Float64(-2.0 * Float64(U_m * 0.5));
      	elseif (t_1 <= 1e+307)
      		tmp = Float64(Float64(cosh(asinh(Float64(U_m / Float64(Float64(J + J) * t_2)))) * Float64(J * -2.0)) * t_2);
      	else
      		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
      	end
      	return tmp
      end
      
      U_m = abs(U);
      function tmp_2 = code(J, K, U_m)
      	t_0 = cos((K / 2.0));
      	t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_0)) ^ 2.0)));
      	t_2 = cos((K * -0.5));
      	tmp = 0.0;
      	if (t_1 <= -Inf)
      		tmp = -2.0 * (U_m * 0.5);
      	elseif (t_1 <= 1e+307)
      		tmp = (cosh(asinh((U_m / ((J + J) * t_2)))) * (J * -2.0)) * t_2;
      	else
      		tmp = -2.0 * (-0.5 * U_m);
      	end
      	tmp_2 = tmp;
      end
      
      U_m = N[Abs[U], $MachinePrecision]
      code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[Cos[N[(K * -0.5), $MachinePrecision]], $MachinePrecision]}, If[LessEqual[t$95$1, (-Infinity)], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$1, 1e+307], N[(N[(N[Cosh[N[ArcSinh[N[(U$95$m / N[(N[(J + J), $MachinePrecision] * t$95$2), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * N[(J * -2.0), $MachinePrecision]), $MachinePrecision] * t$95$2), $MachinePrecision], N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]]
      
      \begin{array}{l}
      U_m = \left|U\right|
      
      \\
      \begin{array}{l}
      t_0 := \cos \left(\frac{K}{2}\right)\\
      t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\
      t_2 := \cos \left(K \cdot -0.5\right)\\
      \mathbf{if}\;t\_1 \leq -\infty:\\
      \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\
      
      \mathbf{elif}\;t\_1 \leq 10^{+307}:\\
      \;\;\;\;\left(\cosh \sinh^{-1} \left(\frac{U\_m}{\left(J + J\right) \cdot t\_2}\right) \cdot \left(J \cdot -2\right)\right) \cdot t\_2\\
      
      \mathbf{else}:\\
      \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
      
      
      \end{array}
      \end{array}
      
      Derivation
      1. Split input into 3 regimes
      2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0

        1. Initial program 73.3%

          \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
        2. Taylor expanded in J around 0

          \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
        3. Step-by-step derivation
          1. lower-*.f64N/A

            \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
          2. lower-*.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
          3. lower-cos.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
          4. lower-*.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          5. lower-sqrt.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          6. lower-*.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          7. lower-/.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          8. lower-pow.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          9. lower-pow.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          10. lower-cos.f64N/A

            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
          11. lower-*.f6414.8

            \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
        4. Applied rewrites14.8%

          \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
        5. Taylor expanded in U around 0

          \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
        6. Step-by-step derivation
          1. lower-*.f64N/A

            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
          2. lower-*.f64N/A

            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
          3. lower-cos.f64N/A

            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
          4. lower-*.f64N/A

            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
          5. lower-sqrt.f64N/A

            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
          6. lower-/.f64N/A

            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
          7. lower-pow.f64N/A

            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
          8. lower-cos.f64N/A

            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
          9. lower-*.f6425.6

            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
        7. Applied rewrites25.6%

          \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
        8. Taylor expanded in K around 0

          \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
        9. Step-by-step derivation
          1. Applied rewrites26.4%

            \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

          if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < 9.99999999999999986e306

          1. Initial program 73.3%

            \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          2. Step-by-step derivation
            1. lift-*.f64N/A

              \[\leadsto \color{blue}{\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
            2. *-commutativeN/A

              \[\leadsto \color{blue}{\sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \cdot \left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right)} \]
            3. lift-*.f64N/A

              \[\leadsto \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \cdot \color{blue}{\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right)} \]
            4. associate-*r*N/A

              \[\leadsto \color{blue}{\left(\sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \cdot \left(-2 \cdot J\right)\right) \cdot \cos \left(\frac{K}{2}\right)} \]
            5. lower-*.f64N/A

              \[\leadsto \color{blue}{\left(\sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \cdot \left(-2 \cdot J\right)\right) \cdot \cos \left(\frac{K}{2}\right)} \]
          3. Applied rewrites84.8%

            \[\leadsto \color{blue}{\left(\cosh \sinh^{-1} \left(\frac{U}{\left(J + J\right) \cdot \cos \left(K \cdot -0.5\right)}\right) \cdot \left(J \cdot -2\right)\right) \cdot \cos \left(K \cdot -0.5\right)} \]

          if 9.99999999999999986e306 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

          1. Initial program 73.3%

            \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          2. Taylor expanded in J around 0

            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
          3. Step-by-step derivation
            1. lower-*.f64N/A

              \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
            2. lower-*.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
            3. lower-cos.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
            4. lower-*.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            5. lower-sqrt.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            6. lower-*.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            7. lower-/.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            8. lower-pow.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            9. lower-pow.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            10. lower-cos.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            11. lower-*.f6414.8

              \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
          4. Applied rewrites14.8%

            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
          5. Taylor expanded in K around 0

            \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
          6. Step-by-step derivation
            1. lower-sqrt.f64N/A

              \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
            2. lower-*.f64N/A

              \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
            3. lower-pow.f6414.9

              \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
          7. Applied rewrites14.9%

            \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
          8. Taylor expanded in U around -inf

            \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
          9. Step-by-step derivation
            1. lower-*.f6426.5

              \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
          10. Applied rewrites26.5%

            \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
        10. Recombined 3 regimes into one program.
        11. Add Preprocessing

        Alternative 4: 98.2% accurate, 0.3× speedup?

        \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\ t_2 := \cos \left(K \cdot -0.5\right)\\ \mathbf{if}\;t\_1 \leq -\infty:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{elif}\;t\_1 \leq 10^{+307}:\\ \;\;\;\;\left(\cosh \sinh^{-1} \left(\frac{U\_m}{\left(J + J\right) \cdot t\_2}\right) \cdot t\_2\right) \cdot \left(J \cdot -2\right)\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
        U_m = (fabs.f64 U)
        (FPCore (J K U_m)
         :precision binary64
         (let* ((t_0 (cos (/ K 2.0)))
                (t_1
                 (*
                  (* (* -2.0 J) t_0)
                  (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_0)) 2.0)))))
                (t_2 (cos (* K -0.5))))
           (if (<= t_1 (- INFINITY))
             (* -2.0 (* U_m 0.5))
             (if (<= t_1 1e+307)
               (* (* (cosh (asinh (/ U_m (* (+ J J) t_2)))) t_2) (* J -2.0))
               (* -2.0 (* -0.5 U_m))))))
        U_m = fabs(U);
        double code(double J, double K, double U_m) {
        	double t_0 = cos((K / 2.0));
        	double t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_0)), 2.0)));
        	double t_2 = cos((K * -0.5));
        	double tmp;
        	if (t_1 <= -((double) INFINITY)) {
        		tmp = -2.0 * (U_m * 0.5);
        	} else if (t_1 <= 1e+307) {
        		tmp = (cosh(asinh((U_m / ((J + J) * t_2)))) * t_2) * (J * -2.0);
        	} else {
        		tmp = -2.0 * (-0.5 * U_m);
        	}
        	return tmp;
        }
        
        U_m = math.fabs(U)
        def code(J, K, U_m):
        	t_0 = math.cos((K / 2.0))
        	t_1 = ((-2.0 * J) * t_0) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_0)), 2.0)))
        	t_2 = math.cos((K * -0.5))
        	tmp = 0
        	if t_1 <= -math.inf:
        		tmp = -2.0 * (U_m * 0.5)
        	elif t_1 <= 1e+307:
        		tmp = (math.cosh(math.asinh((U_m / ((J + J) * t_2)))) * t_2) * (J * -2.0)
        	else:
        		tmp = -2.0 * (-0.5 * U_m)
        	return tmp
        
        U_m = abs(U)
        function code(J, K, U_m)
        	t_0 = cos(Float64(K / 2.0))
        	t_1 = Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))))
        	t_2 = cos(Float64(K * -0.5))
        	tmp = 0.0
        	if (t_1 <= Float64(-Inf))
        		tmp = Float64(-2.0 * Float64(U_m * 0.5));
        	elseif (t_1 <= 1e+307)
        		tmp = Float64(Float64(cosh(asinh(Float64(U_m / Float64(Float64(J + J) * t_2)))) * t_2) * Float64(J * -2.0));
        	else
        		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
        	end
        	return tmp
        end
        
        U_m = abs(U);
        function tmp_2 = code(J, K, U_m)
        	t_0 = cos((K / 2.0));
        	t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_0)) ^ 2.0)));
        	t_2 = cos((K * -0.5));
        	tmp = 0.0;
        	if (t_1 <= -Inf)
        		tmp = -2.0 * (U_m * 0.5);
        	elseif (t_1 <= 1e+307)
        		tmp = (cosh(asinh((U_m / ((J + J) * t_2)))) * t_2) * (J * -2.0);
        	else
        		tmp = -2.0 * (-0.5 * U_m);
        	end
        	tmp_2 = tmp;
        end
        
        U_m = N[Abs[U], $MachinePrecision]
        code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[Cos[N[(K * -0.5), $MachinePrecision]], $MachinePrecision]}, If[LessEqual[t$95$1, (-Infinity)], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$1, 1e+307], N[(N[(N[Cosh[N[ArcSinh[N[(U$95$m / N[(N[(J + J), $MachinePrecision] * t$95$2), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * t$95$2), $MachinePrecision] * N[(J * -2.0), $MachinePrecision]), $MachinePrecision], N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]]
        
        \begin{array}{l}
        U_m = \left|U\right|
        
        \\
        \begin{array}{l}
        t_0 := \cos \left(\frac{K}{2}\right)\\
        t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\
        t_2 := \cos \left(K \cdot -0.5\right)\\
        \mathbf{if}\;t\_1 \leq -\infty:\\
        \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\
        
        \mathbf{elif}\;t\_1 \leq 10^{+307}:\\
        \;\;\;\;\left(\cosh \sinh^{-1} \left(\frac{U\_m}{\left(J + J\right) \cdot t\_2}\right) \cdot t\_2\right) \cdot \left(J \cdot -2\right)\\
        
        \mathbf{else}:\\
        \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
        
        
        \end{array}
        \end{array}
        
        Derivation
        1. Split input into 3 regimes
        2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0

          1. Initial program 73.3%

            \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
          2. Taylor expanded in J around 0

            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
          3. Step-by-step derivation
            1. lower-*.f64N/A

              \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
            2. lower-*.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
            3. lower-cos.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
            4. lower-*.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            5. lower-sqrt.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            6. lower-*.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            7. lower-/.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            8. lower-pow.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            9. lower-pow.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            10. lower-cos.f64N/A

              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
            11. lower-*.f6414.8

              \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
          4. Applied rewrites14.8%

            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
          5. Taylor expanded in U around 0

            \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
          6. Step-by-step derivation
            1. lower-*.f64N/A

              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
            2. lower-*.f64N/A

              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
            3. lower-cos.f64N/A

              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
            4. lower-*.f64N/A

              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
            5. lower-sqrt.f64N/A

              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
            6. lower-/.f64N/A

              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
            7. lower-pow.f64N/A

              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
            8. lower-cos.f64N/A

              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
            9. lower-*.f6425.6

              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
          7. Applied rewrites25.6%

            \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
          8. Taylor expanded in K around 0

            \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
          9. Step-by-step derivation
            1. Applied rewrites26.4%

              \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

            if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < 9.99999999999999986e306

            1. Initial program 73.3%

              \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
            2. Step-by-step derivation
              1. lift-*.f64N/A

                \[\leadsto \color{blue}{\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
              2. lift-*.f64N/A

                \[\leadsto \color{blue}{\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
              3. associate-*l*N/A

                \[\leadsto \color{blue}{\left(-2 \cdot J\right) \cdot \left(\cos \left(\frac{K}{2}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}\right)} \]
              4. *-commutativeN/A

                \[\leadsto \color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}\right) \cdot \left(-2 \cdot J\right)} \]
              5. lower-*.f64N/A

                \[\leadsto \color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}\right) \cdot \left(-2 \cdot J\right)} \]
            3. Applied rewrites84.8%

              \[\leadsto \color{blue}{\left(\cosh \sinh^{-1} \left(\frac{U}{\left(J + J\right) \cdot \cos \left(K \cdot -0.5\right)}\right) \cdot \cos \left(K \cdot -0.5\right)\right) \cdot \left(J \cdot -2\right)} \]

            if 9.99999999999999986e306 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

            1. Initial program 73.3%

              \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
            2. Taylor expanded in J around 0

              \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
            3. Step-by-step derivation
              1. lower-*.f64N/A

                \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
              2. lower-*.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
              3. lower-cos.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
              4. lower-*.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              5. lower-sqrt.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              6. lower-*.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              7. lower-/.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              8. lower-pow.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              9. lower-pow.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              10. lower-cos.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              11. lower-*.f6414.8

                \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
            4. Applied rewrites14.8%

              \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
            5. Taylor expanded in K around 0

              \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
            6. Step-by-step derivation
              1. lower-sqrt.f64N/A

                \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
              2. lower-*.f64N/A

                \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
              3. lower-pow.f6414.9

                \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
            7. Applied rewrites14.9%

              \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
            8. Taylor expanded in U around -inf

              \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
            9. Step-by-step derivation
              1. lower-*.f6426.5

                \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
            10. Applied rewrites26.5%

              \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
          10. Recombined 3 regimes into one program.
          11. Add Preprocessing

          Alternative 5: 91.3% accurate, 0.4× speedup?

          \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ t_1 := \left(-2 \cdot J\right) \cdot t\_0\\ t_2 := t\_1 \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\ \mathbf{if}\;t\_2 \leq -\infty:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{elif}\;t\_2 \leq 10^{+307}:\\ \;\;\;\;t\_1 \cdot \sqrt{1 + {\left(0.5 \cdot \frac{U\_m}{J}\right)}^{2}}\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
          U_m = (fabs.f64 U)
          (FPCore (J K U_m)
           :precision binary64
           (let* ((t_0 (cos (/ K 2.0)))
                  (t_1 (* (* -2.0 J) t_0))
                  (t_2 (* t_1 (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_0)) 2.0))))))
             (if (<= t_2 (- INFINITY))
               (* -2.0 (* U_m 0.5))
               (if (<= t_2 1e+307)
                 (* t_1 (sqrt (+ 1.0 (pow (* 0.5 (/ U_m J)) 2.0))))
                 (* -2.0 (* -0.5 U_m))))))
          U_m = fabs(U);
          double code(double J, double K, double U_m) {
          	double t_0 = cos((K / 2.0));
          	double t_1 = (-2.0 * J) * t_0;
          	double t_2 = t_1 * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_0)), 2.0)));
          	double tmp;
          	if (t_2 <= -((double) INFINITY)) {
          		tmp = -2.0 * (U_m * 0.5);
          	} else if (t_2 <= 1e+307) {
          		tmp = t_1 * sqrt((1.0 + pow((0.5 * (U_m / J)), 2.0)));
          	} else {
          		tmp = -2.0 * (-0.5 * U_m);
          	}
          	return tmp;
          }
          
          U_m = Math.abs(U);
          public static double code(double J, double K, double U_m) {
          	double t_0 = Math.cos((K / 2.0));
          	double t_1 = (-2.0 * J) * t_0;
          	double t_2 = t_1 * Math.sqrt((1.0 + Math.pow((U_m / ((2.0 * J) * t_0)), 2.0)));
          	double tmp;
          	if (t_2 <= -Double.POSITIVE_INFINITY) {
          		tmp = -2.0 * (U_m * 0.5);
          	} else if (t_2 <= 1e+307) {
          		tmp = t_1 * Math.sqrt((1.0 + Math.pow((0.5 * (U_m / J)), 2.0)));
          	} else {
          		tmp = -2.0 * (-0.5 * U_m);
          	}
          	return tmp;
          }
          
          U_m = math.fabs(U)
          def code(J, K, U_m):
          	t_0 = math.cos((K / 2.0))
          	t_1 = (-2.0 * J) * t_0
          	t_2 = t_1 * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_0)), 2.0)))
          	tmp = 0
          	if t_2 <= -math.inf:
          		tmp = -2.0 * (U_m * 0.5)
          	elif t_2 <= 1e+307:
          		tmp = t_1 * math.sqrt((1.0 + math.pow((0.5 * (U_m / J)), 2.0)))
          	else:
          		tmp = -2.0 * (-0.5 * U_m)
          	return tmp
          
          U_m = abs(U)
          function code(J, K, U_m)
          	t_0 = cos(Float64(K / 2.0))
          	t_1 = Float64(Float64(-2.0 * J) * t_0)
          	t_2 = Float64(t_1 * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))))
          	tmp = 0.0
          	if (t_2 <= Float64(-Inf))
          		tmp = Float64(-2.0 * Float64(U_m * 0.5));
          	elseif (t_2 <= 1e+307)
          		tmp = Float64(t_1 * sqrt(Float64(1.0 + (Float64(0.5 * Float64(U_m / J)) ^ 2.0))));
          	else
          		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
          	end
          	return tmp
          end
          
          U_m = abs(U);
          function tmp_2 = code(J, K, U_m)
          	t_0 = cos((K / 2.0));
          	t_1 = (-2.0 * J) * t_0;
          	t_2 = t_1 * sqrt((1.0 + ((U_m / ((2.0 * J) * t_0)) ^ 2.0)));
          	tmp = 0.0;
          	if (t_2 <= -Inf)
          		tmp = -2.0 * (U_m * 0.5);
          	elseif (t_2 <= 1e+307)
          		tmp = t_1 * sqrt((1.0 + ((0.5 * (U_m / J)) ^ 2.0)));
          	else
          		tmp = -2.0 * (-0.5 * U_m);
          	end
          	tmp_2 = tmp;
          end
          
          U_m = N[Abs[U], $MachinePrecision]
          code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]}, Block[{t$95$2 = N[(t$95$1 * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$2, (-Infinity)], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$2, 1e+307], N[(t$95$1 * N[Sqrt[N[(1.0 + N[Power[N[(0.5 * N[(U$95$m / J), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]]
          
          \begin{array}{l}
          U_m = \left|U\right|
          
          \\
          \begin{array}{l}
          t_0 := \cos \left(\frac{K}{2}\right)\\
          t_1 := \left(-2 \cdot J\right) \cdot t\_0\\
          t_2 := t\_1 \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\
          \mathbf{if}\;t\_2 \leq -\infty:\\
          \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\
          
          \mathbf{elif}\;t\_2 \leq 10^{+307}:\\
          \;\;\;\;t\_1 \cdot \sqrt{1 + {\left(0.5 \cdot \frac{U\_m}{J}\right)}^{2}}\\
          
          \mathbf{else}:\\
          \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
          
          
          \end{array}
          \end{array}
          
          Derivation
          1. Split input into 3 regimes
          2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0

            1. Initial program 73.3%

              \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
            2. Taylor expanded in J around 0

              \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
            3. Step-by-step derivation
              1. lower-*.f64N/A

                \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
              2. lower-*.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
              3. lower-cos.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
              4. lower-*.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              5. lower-sqrt.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              6. lower-*.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              7. lower-/.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              8. lower-pow.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              9. lower-pow.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              10. lower-cos.f64N/A

                \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
              11. lower-*.f6414.8

                \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
            4. Applied rewrites14.8%

              \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
            5. Taylor expanded in U around 0

              \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
            6. Step-by-step derivation
              1. lower-*.f64N/A

                \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
              2. lower-*.f64N/A

                \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
              3. lower-cos.f64N/A

                \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
              4. lower-*.f64N/A

                \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
              5. lower-sqrt.f64N/A

                \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
              6. lower-/.f64N/A

                \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
              7. lower-pow.f64N/A

                \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
              8. lower-cos.f64N/A

                \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
              9. lower-*.f6425.6

                \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
            7. Applied rewrites25.6%

              \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
            8. Taylor expanded in K around 0

              \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
            9. Step-by-step derivation
              1. Applied rewrites26.4%

                \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

              if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < 9.99999999999999986e306

              1. Initial program 73.3%

                \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
              2. Taylor expanded in K around 0

                \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\color{blue}{\left(\frac{1}{2} \cdot \frac{U}{J}\right)}}^{2}} \]
              3. Step-by-step derivation
                1. lower-*.f64N/A

                  \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{1}{2} \cdot \color{blue}{\frac{U}{J}}\right)}^{2}} \]
                2. lower-/.f6464.9

                  \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(0.5 \cdot \frac{U}{\color{blue}{J}}\right)}^{2}} \]
              4. Applied rewrites64.9%

                \[\leadsto \left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\color{blue}{\left(0.5 \cdot \frac{U}{J}\right)}}^{2}} \]

              if 9.99999999999999986e306 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

              1. Initial program 73.3%

                \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
              2. Taylor expanded in J around 0

                \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
              3. Step-by-step derivation
                1. lower-*.f64N/A

                  \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                2. lower-*.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                3. lower-cos.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                4. lower-*.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                5. lower-sqrt.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                6. lower-*.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                7. lower-/.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                8. lower-pow.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                9. lower-pow.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                10. lower-cos.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                11. lower-*.f6414.8

                  \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
              4. Applied rewrites14.8%

                \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
              5. Taylor expanded in K around 0

                \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
              6. Step-by-step derivation
                1. lower-sqrt.f64N/A

                  \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                2. lower-*.f64N/A

                  \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                3. lower-pow.f6414.9

                  \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
              7. Applied rewrites14.9%

                \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
              8. Taylor expanded in U around -inf

                \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
              9. Step-by-step derivation
                1. lower-*.f6426.5

                  \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
              10. Applied rewrites26.5%

                \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
            10. Recombined 3 regimes into one program.
            11. Add Preprocessing

            Alternative 6: 90.5% accurate, 0.4× speedup?

            \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\ \mathbf{if}\;t\_1 \leq -\infty:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{elif}\;t\_1 \leq 10^{+307}:\\ \;\;\;\;\left(\left(\cos \left(K \cdot -0.5\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(0.5 \cdot \frac{U\_m}{J}\right)\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
            U_m = (fabs.f64 U)
            (FPCore (J K U_m)
             :precision binary64
             (let* ((t_0 (cos (/ K 2.0)))
                    (t_1
                     (*
                      (* (* -2.0 J) t_0)
                      (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_0)) 2.0))))))
               (if (<= t_1 (- INFINITY))
                 (* -2.0 (* U_m 0.5))
                 (if (<= t_1 1e+307)
                   (* (* (* (cos (* K -0.5)) -2.0) J) (cosh (asinh (* 0.5 (/ U_m J)))))
                   (* -2.0 (* -0.5 U_m))))))
            U_m = fabs(U);
            double code(double J, double K, double U_m) {
            	double t_0 = cos((K / 2.0));
            	double t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_0)), 2.0)));
            	double tmp;
            	if (t_1 <= -((double) INFINITY)) {
            		tmp = -2.0 * (U_m * 0.5);
            	} else if (t_1 <= 1e+307) {
            		tmp = ((cos((K * -0.5)) * -2.0) * J) * cosh(asinh((0.5 * (U_m / J))));
            	} else {
            		tmp = -2.0 * (-0.5 * U_m);
            	}
            	return tmp;
            }
            
            U_m = math.fabs(U)
            def code(J, K, U_m):
            	t_0 = math.cos((K / 2.0))
            	t_1 = ((-2.0 * J) * t_0) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_0)), 2.0)))
            	tmp = 0
            	if t_1 <= -math.inf:
            		tmp = -2.0 * (U_m * 0.5)
            	elif t_1 <= 1e+307:
            		tmp = ((math.cos((K * -0.5)) * -2.0) * J) * math.cosh(math.asinh((0.5 * (U_m / J))))
            	else:
            		tmp = -2.0 * (-0.5 * U_m)
            	return tmp
            
            U_m = abs(U)
            function code(J, K, U_m)
            	t_0 = cos(Float64(K / 2.0))
            	t_1 = Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))))
            	tmp = 0.0
            	if (t_1 <= Float64(-Inf))
            		tmp = Float64(-2.0 * Float64(U_m * 0.5));
            	elseif (t_1 <= 1e+307)
            		tmp = Float64(Float64(Float64(cos(Float64(K * -0.5)) * -2.0) * J) * cosh(asinh(Float64(0.5 * Float64(U_m / J)))));
            	else
            		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
            	end
            	return tmp
            end
            
            U_m = abs(U);
            function tmp_2 = code(J, K, U_m)
            	t_0 = cos((K / 2.0));
            	t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_0)) ^ 2.0)));
            	tmp = 0.0;
            	if (t_1 <= -Inf)
            		tmp = -2.0 * (U_m * 0.5);
            	elseif (t_1 <= 1e+307)
            		tmp = ((cos((K * -0.5)) * -2.0) * J) * cosh(asinh((0.5 * (U_m / J))));
            	else
            		tmp = -2.0 * (-0.5 * U_m);
            	end
            	tmp_2 = tmp;
            end
            
            U_m = N[Abs[U], $MachinePrecision]
            code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$1, (-Infinity)], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$1, 1e+307], N[(N[(N[(N[Cos[N[(K * -0.5), $MachinePrecision]], $MachinePrecision] * -2.0), $MachinePrecision] * J), $MachinePrecision] * N[Cosh[N[ArcSinh[N[(0.5 * N[(U$95$m / J), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision], N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]
            
            \begin{array}{l}
            U_m = \left|U\right|
            
            \\
            \begin{array}{l}
            t_0 := \cos \left(\frac{K}{2}\right)\\
            t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\
            \mathbf{if}\;t\_1 \leq -\infty:\\
            \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\
            
            \mathbf{elif}\;t\_1 \leq 10^{+307}:\\
            \;\;\;\;\left(\left(\cos \left(K \cdot -0.5\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(0.5 \cdot \frac{U\_m}{J}\right)\\
            
            \mathbf{else}:\\
            \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
            
            
            \end{array}
            \end{array}
            
            Derivation
            1. Split input into 3 regimes
            2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0

              1. Initial program 73.3%

                \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
              2. Taylor expanded in J around 0

                \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
              3. Step-by-step derivation
                1. lower-*.f64N/A

                  \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                2. lower-*.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                3. lower-cos.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                4. lower-*.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                5. lower-sqrt.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                6. lower-*.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                7. lower-/.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                8. lower-pow.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                9. lower-pow.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                10. lower-cos.f64N/A

                  \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                11. lower-*.f6414.8

                  \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
              4. Applied rewrites14.8%

                \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
              5. Taylor expanded in U around 0

                \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
              6. Step-by-step derivation
                1. lower-*.f64N/A

                  \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
                2. lower-*.f64N/A

                  \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                3. lower-cos.f64N/A

                  \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                4. lower-*.f64N/A

                  \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                5. lower-sqrt.f64N/A

                  \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                6. lower-/.f64N/A

                  \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                7. lower-pow.f64N/A

                  \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                8. lower-cos.f64N/A

                  \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                9. lower-*.f6425.6

                  \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
              7. Applied rewrites25.6%

                \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
              8. Taylor expanded in K around 0

                \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
              9. Step-by-step derivation
                1. Applied rewrites26.4%

                  \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

                if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < 9.99999999999999986e306

                1. Initial program 73.3%

                  \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                2. Step-by-step derivation
                  1. lift-*.f64N/A

                    \[\leadsto \color{blue}{\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  2. *-commutativeN/A

                    \[\leadsto \color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot \left(-2 \cdot J\right)\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  3. lift-*.f64N/A

                    \[\leadsto \left(\cos \left(\frac{K}{2}\right) \cdot \color{blue}{\left(-2 \cdot J\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  4. associate-*r*N/A

                    \[\leadsto \color{blue}{\left(\left(\cos \left(\frac{K}{2}\right) \cdot -2\right) \cdot J\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  5. lower-*.f64N/A

                    \[\leadsto \color{blue}{\left(\left(\cos \left(\frac{K}{2}\right) \cdot -2\right) \cdot J\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  6. lower-*.f6473.4

                    \[\leadsto \left(\color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot -2\right)} \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  7. lift-cos.f64N/A

                    \[\leadsto \left(\left(\color{blue}{\cos \left(\frac{K}{2}\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  8. cos-neg-revN/A

                    \[\leadsto \left(\left(\color{blue}{\cos \left(\mathsf{neg}\left(\frac{K}{2}\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  9. lower-cos.f64N/A

                    \[\leadsto \left(\left(\color{blue}{\cos \left(\mathsf{neg}\left(\frac{K}{2}\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  10. lift-/.f64N/A

                    \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(\color{blue}{\frac{K}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  11. mult-flipN/A

                    \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(\color{blue}{K \cdot \frac{1}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  12. metadata-evalN/A

                    \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(K \cdot \color{blue}{\frac{1}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  13. distribute-rgt-neg-inN/A

                    \[\leadsto \left(\left(\cos \color{blue}{\left(K \cdot \left(\mathsf{neg}\left(\frac{1}{2}\right)\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  14. metadata-evalN/A

                    \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{\frac{-1}{2}}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  15. metadata-evalN/A

                    \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{\frac{1}{-2}}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  16. lower-*.f64N/A

                    \[\leadsto \left(\left(\cos \color{blue}{\left(K \cdot \frac{1}{-2}\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  17. metadata-eval73.4

                    \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{-0.5}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  18. lift-sqrt.f64N/A

                    \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \color{blue}{\sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
                  19. lift-+.f64N/A

                    \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{\color{blue}{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
                3. Applied rewrites84.8%

                  \[\leadsto \color{blue}{\left(\left(\cos \left(K \cdot -0.5\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U}{\left(J + J\right) \cdot \cos \left(K \cdot -0.5\right)}\right)} \]
                4. Taylor expanded in K around 0

                  \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \color{blue}{\left(\frac{1}{2} \cdot \frac{U}{J}\right)} \]
                5. Step-by-step derivation
                  1. lower-*.f64N/A

                    \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{1}{2} \cdot \color{blue}{\frac{U}{J}}\right) \]
                  2. lower-/.f6472.2

                    \[\leadsto \left(\left(\cos \left(K \cdot -0.5\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(0.5 \cdot \frac{U}{\color{blue}{J}}\right) \]
                6. Applied rewrites72.2%

                  \[\leadsto \left(\left(\cos \left(K \cdot -0.5\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \color{blue}{\left(0.5 \cdot \frac{U}{J}\right)} \]

                if 9.99999999999999986e306 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

                1. Initial program 73.3%

                  \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                2. Taylor expanded in J around 0

                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                3. Step-by-step derivation
                  1. lower-*.f64N/A

                    \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                  2. lower-*.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                  3. lower-cos.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                  4. lower-*.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  5. lower-sqrt.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  6. lower-*.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  7. lower-/.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  8. lower-pow.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  9. lower-pow.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  10. lower-cos.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  11. lower-*.f6414.8

                    \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                4. Applied rewrites14.8%

                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                5. Taylor expanded in K around 0

                  \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                6. Step-by-step derivation
                  1. lower-sqrt.f64N/A

                    \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                  2. lower-*.f64N/A

                    \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                  3. lower-pow.f6414.9

                    \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                7. Applied rewrites14.9%

                  \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                8. Taylor expanded in U around -inf

                  \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                9. Step-by-step derivation
                  1. lower-*.f6426.5

                    \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                10. Applied rewrites26.5%

                  \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
              10. Recombined 3 regimes into one program.
              11. Add Preprocessing

              Alternative 7: 79.5% accurate, 0.2× speedup?

              \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\ t_2 := -2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right)\\ \mathbf{if}\;t\_1 \leq -\infty:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{elif}\;t\_1 \leq -2 \cdot 10^{+66}:\\ \;\;\;\;t\_2\\ \mathbf{elif}\;t\_1 \leq -5 \cdot 10^{-153}:\\ \;\;\;\;\left(-2 \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U\_m}{\left(J + J\right) \cdot \cos \left(K \cdot -0.5\right)}\right)\\ \mathbf{elif}\;t\_1 \leq 10^{+307}:\\ \;\;\;\;t\_2\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
              U_m = (fabs.f64 U)
              (FPCore (J K U_m)
               :precision binary64
               (let* ((t_0 (cos (/ K 2.0)))
                      (t_1
                       (*
                        (* (* -2.0 J) t_0)
                        (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_0)) 2.0)))))
                      (t_2 (* -2.0 (* J (cos (* 0.5 K))))))
                 (if (<= t_1 (- INFINITY))
                   (* -2.0 (* U_m 0.5))
                   (if (<= t_1 -2e+66)
                     t_2
                     (if (<= t_1 -5e-153)
                       (* (* -2.0 J) (cosh (asinh (/ U_m (* (+ J J) (cos (* K -0.5)))))))
                       (if (<= t_1 1e+307) t_2 (* -2.0 (* -0.5 U_m))))))))
              U_m = fabs(U);
              double code(double J, double K, double U_m) {
              	double t_0 = cos((K / 2.0));
              	double t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_0)), 2.0)));
              	double t_2 = -2.0 * (J * cos((0.5 * K)));
              	double tmp;
              	if (t_1 <= -((double) INFINITY)) {
              		tmp = -2.0 * (U_m * 0.5);
              	} else if (t_1 <= -2e+66) {
              		tmp = t_2;
              	} else if (t_1 <= -5e-153) {
              		tmp = (-2.0 * J) * cosh(asinh((U_m / ((J + J) * cos((K * -0.5))))));
              	} else if (t_1 <= 1e+307) {
              		tmp = t_2;
              	} else {
              		tmp = -2.0 * (-0.5 * U_m);
              	}
              	return tmp;
              }
              
              U_m = math.fabs(U)
              def code(J, K, U_m):
              	t_0 = math.cos((K / 2.0))
              	t_1 = ((-2.0 * J) * t_0) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_0)), 2.0)))
              	t_2 = -2.0 * (J * math.cos((0.5 * K)))
              	tmp = 0
              	if t_1 <= -math.inf:
              		tmp = -2.0 * (U_m * 0.5)
              	elif t_1 <= -2e+66:
              		tmp = t_2
              	elif t_1 <= -5e-153:
              		tmp = (-2.0 * J) * math.cosh(math.asinh((U_m / ((J + J) * math.cos((K * -0.5))))))
              	elif t_1 <= 1e+307:
              		tmp = t_2
              	else:
              		tmp = -2.0 * (-0.5 * U_m)
              	return tmp
              
              U_m = abs(U)
              function code(J, K, U_m)
              	t_0 = cos(Float64(K / 2.0))
              	t_1 = Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))))
              	t_2 = Float64(-2.0 * Float64(J * cos(Float64(0.5 * K))))
              	tmp = 0.0
              	if (t_1 <= Float64(-Inf))
              		tmp = Float64(-2.0 * Float64(U_m * 0.5));
              	elseif (t_1 <= -2e+66)
              		tmp = t_2;
              	elseif (t_1 <= -5e-153)
              		tmp = Float64(Float64(-2.0 * J) * cosh(asinh(Float64(U_m / Float64(Float64(J + J) * cos(Float64(K * -0.5)))))));
              	elseif (t_1 <= 1e+307)
              		tmp = t_2;
              	else
              		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
              	end
              	return tmp
              end
              
              U_m = abs(U);
              function tmp_2 = code(J, K, U_m)
              	t_0 = cos((K / 2.0));
              	t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_0)) ^ 2.0)));
              	t_2 = -2.0 * (J * cos((0.5 * K)));
              	tmp = 0.0;
              	if (t_1 <= -Inf)
              		tmp = -2.0 * (U_m * 0.5);
              	elseif (t_1 <= -2e+66)
              		tmp = t_2;
              	elseif (t_1 <= -5e-153)
              		tmp = (-2.0 * J) * cosh(asinh((U_m / ((J + J) * cos((K * -0.5))))));
              	elseif (t_1 <= 1e+307)
              		tmp = t_2;
              	else
              		tmp = -2.0 * (-0.5 * U_m);
              	end
              	tmp_2 = tmp;
              end
              
              U_m = N[Abs[U], $MachinePrecision]
              code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[(-2.0 * N[(J * N[Cos[N[(0.5 * K), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$1, (-Infinity)], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$1, -2e+66], t$95$2, If[LessEqual[t$95$1, -5e-153], N[(N[(-2.0 * J), $MachinePrecision] * N[Cosh[N[ArcSinh[N[(U$95$m / N[(N[(J + J), $MachinePrecision] * N[Cos[N[(K * -0.5), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$1, 1e+307], t$95$2, N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]]]]
              
              \begin{array}{l}
              U_m = \left|U\right|
              
              \\
              \begin{array}{l}
              t_0 := \cos \left(\frac{K}{2}\right)\\
              t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\
              t_2 := -2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right)\\
              \mathbf{if}\;t\_1 \leq -\infty:\\
              \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\
              
              \mathbf{elif}\;t\_1 \leq -2 \cdot 10^{+66}:\\
              \;\;\;\;t\_2\\
              
              \mathbf{elif}\;t\_1 \leq -5 \cdot 10^{-153}:\\
              \;\;\;\;\left(-2 \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U\_m}{\left(J + J\right) \cdot \cos \left(K \cdot -0.5\right)}\right)\\
              
              \mathbf{elif}\;t\_1 \leq 10^{+307}:\\
              \;\;\;\;t\_2\\
              
              \mathbf{else}:\\
              \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
              
              
              \end{array}
              \end{array}
              
              Derivation
              1. Split input into 4 regimes
              2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0

                1. Initial program 73.3%

                  \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                2. Taylor expanded in J around 0

                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                3. Step-by-step derivation
                  1. lower-*.f64N/A

                    \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                  2. lower-*.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                  3. lower-cos.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                  4. lower-*.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  5. lower-sqrt.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  6. lower-*.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  7. lower-/.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  8. lower-pow.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  9. lower-pow.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  10. lower-cos.f64N/A

                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                  11. lower-*.f6414.8

                    \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                4. Applied rewrites14.8%

                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                5. Taylor expanded in U around 0

                  \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
                6. Step-by-step derivation
                  1. lower-*.f64N/A

                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
                  2. lower-*.f64N/A

                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                  3. lower-cos.f64N/A

                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                  4. lower-*.f64N/A

                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                  5. lower-sqrt.f64N/A

                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                  6. lower-/.f64N/A

                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                  7. lower-pow.f64N/A

                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                  8. lower-cos.f64N/A

                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                  9. lower-*.f6425.6

                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
                7. Applied rewrites25.6%

                  \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
                8. Taylor expanded in K around 0

                  \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
                9. Step-by-step derivation
                  1. Applied rewrites26.4%

                    \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

                  if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -1.99999999999999989e66 or -5.00000000000000033e-153 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < 9.99999999999999986e306

                  1. Initial program 73.3%

                    \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  2. Taylor expanded in J around 0

                    \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                  3. Step-by-step derivation
                    1. lower-*.f64N/A

                      \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                    2. lower-*.f64N/A

                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                    3. lower-cos.f64N/A

                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                    4. lower-*.f64N/A

                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                    5. lower-sqrt.f64N/A

                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                    6. lower-*.f64N/A

                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                    7. lower-/.f64N/A

                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                    8. lower-pow.f64N/A

                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                    9. lower-pow.f64N/A

                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                    10. lower-cos.f64N/A

                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                    11. lower-*.f6414.8

                      \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                  4. Applied rewrites14.8%

                    \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                  5. Taylor expanded in K around 0

                    \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                  6. Step-by-step derivation
                    1. lower-sqrt.f64N/A

                      \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                    2. lower-*.f64N/A

                      \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                    3. lower-pow.f6414.9

                      \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                  7. Applied rewrites14.9%

                    \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                  8. Taylor expanded in U around -inf

                    \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                  9. Step-by-step derivation
                    1. lower-*.f6426.5

                      \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                  10. Applied rewrites26.5%

                    \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                  11. Taylor expanded in J around inf

                    \[\leadsto \color{blue}{-2 \cdot \left(J \cdot \cos \left(\frac{1}{2} \cdot K\right)\right)} \]
                  12. Step-by-step derivation
                    1. lower-*.f64N/A

                      \[\leadsto -2 \cdot \color{blue}{\left(J \cdot \cos \left(\frac{1}{2} \cdot K\right)\right)} \]
                    2. lower-*.f64N/A

                      \[\leadsto -2 \cdot \left(J \cdot \color{blue}{\cos \left(\frac{1}{2} \cdot K\right)}\right) \]
                    3. lower-cos.f64N/A

                      \[\leadsto -2 \cdot \left(J \cdot \cos \left(\frac{1}{2} \cdot K\right)\right) \]
                    4. lower-*.f6452.4

                      \[\leadsto -2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right) \]
                  13. Applied rewrites52.4%

                    \[\leadsto \color{blue}{-2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right)} \]

                  if -1.99999999999999989e66 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -5.00000000000000033e-153

                  1. Initial program 73.3%

                    \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                  2. Step-by-step derivation
                    1. lift-*.f64N/A

                      \[\leadsto \color{blue}{\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    2. *-commutativeN/A

                      \[\leadsto \color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot \left(-2 \cdot J\right)\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    3. lift-*.f64N/A

                      \[\leadsto \left(\cos \left(\frac{K}{2}\right) \cdot \color{blue}{\left(-2 \cdot J\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    4. associate-*r*N/A

                      \[\leadsto \color{blue}{\left(\left(\cos \left(\frac{K}{2}\right) \cdot -2\right) \cdot J\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    5. lower-*.f64N/A

                      \[\leadsto \color{blue}{\left(\left(\cos \left(\frac{K}{2}\right) \cdot -2\right) \cdot J\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    6. lower-*.f6473.4

                      \[\leadsto \left(\color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot -2\right)} \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    7. lift-cos.f64N/A

                      \[\leadsto \left(\left(\color{blue}{\cos \left(\frac{K}{2}\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    8. cos-neg-revN/A

                      \[\leadsto \left(\left(\color{blue}{\cos \left(\mathsf{neg}\left(\frac{K}{2}\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    9. lower-cos.f64N/A

                      \[\leadsto \left(\left(\color{blue}{\cos \left(\mathsf{neg}\left(\frac{K}{2}\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    10. lift-/.f64N/A

                      \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(\color{blue}{\frac{K}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    11. mult-flipN/A

                      \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(\color{blue}{K \cdot \frac{1}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    12. metadata-evalN/A

                      \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(K \cdot \color{blue}{\frac{1}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    13. distribute-rgt-neg-inN/A

                      \[\leadsto \left(\left(\cos \color{blue}{\left(K \cdot \left(\mathsf{neg}\left(\frac{1}{2}\right)\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    14. metadata-evalN/A

                      \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{\frac{-1}{2}}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    15. metadata-evalN/A

                      \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{\frac{1}{-2}}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    16. lower-*.f64N/A

                      \[\leadsto \left(\left(\cos \color{blue}{\left(K \cdot \frac{1}{-2}\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    17. metadata-eval73.4

                      \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{-0.5}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    18. lift-sqrt.f64N/A

                      \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \color{blue}{\sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
                    19. lift-+.f64N/A

                      \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{\color{blue}{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
                  3. Applied rewrites84.8%

                    \[\leadsto \color{blue}{\left(\left(\cos \left(K \cdot -0.5\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U}{\left(J + J\right) \cdot \cos \left(K \cdot -0.5\right)}\right)} \]
                  4. Taylor expanded in K around 0

                    \[\leadsto \left(\color{blue}{-2} \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U}{\left(J + J\right) \cdot \cos \left(K \cdot \frac{-1}{2}\right)}\right) \]
                  5. Step-by-step derivation
                    1. Applied rewrites47.6%

                      \[\leadsto \left(\color{blue}{-2} \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U}{\left(J + J\right) \cdot \cos \left(K \cdot -0.5\right)}\right) \]

                    if 9.99999999999999986e306 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

                    1. Initial program 73.3%

                      \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    2. Taylor expanded in J around 0

                      \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                    3. Step-by-step derivation
                      1. lower-*.f64N/A

                        \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                      2. lower-*.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                      3. lower-cos.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                      4. lower-*.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      5. lower-sqrt.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      6. lower-*.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      7. lower-/.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      8. lower-pow.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      9. lower-pow.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      10. lower-cos.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      11. lower-*.f6414.8

                        \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                    4. Applied rewrites14.8%

                      \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                    5. Taylor expanded in K around 0

                      \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                    6. Step-by-step derivation
                      1. lower-sqrt.f64N/A

                        \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                      2. lower-*.f64N/A

                        \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                      3. lower-pow.f6414.9

                        \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                    7. Applied rewrites14.9%

                      \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                    8. Taylor expanded in U around -inf

                      \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                    9. Step-by-step derivation
                      1. lower-*.f6426.5

                        \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                    10. Applied rewrites26.5%

                      \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                  6. Recombined 4 regimes into one program.
                  7. Add Preprocessing

                  Alternative 8: 77.8% accurate, 0.2× speedup?

                  \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\ t_2 := -2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right)\\ \mathbf{if}\;t\_1 \leq -\infty:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{elif}\;t\_1 \leq -1 \cdot 10^{+60}:\\ \;\;\;\;t\_2\\ \mathbf{elif}\;t\_1 \leq -5 \cdot 10^{-153}:\\ \;\;\;\;\left(\mathsf{fma}\left(\mathsf{fma}\left(0.0026041666666666665, K \cdot K, -0.125\right), K \cdot K, 1\right) \cdot \left(J \cdot -2\right)\right) \cdot \sqrt{{\left(0.5 \cdot \frac{U\_m}{J}\right)}^{2} + 1}\\ \mathbf{elif}\;t\_1 \leq 10^{+307}:\\ \;\;\;\;t\_2\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
                  U_m = (fabs.f64 U)
                  (FPCore (J K U_m)
                   :precision binary64
                   (let* ((t_0 (cos (/ K 2.0)))
                          (t_1
                           (*
                            (* (* -2.0 J) t_0)
                            (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_0)) 2.0)))))
                          (t_2 (* -2.0 (* J (cos (* 0.5 K))))))
                     (if (<= t_1 (- INFINITY))
                       (* -2.0 (* U_m 0.5))
                       (if (<= t_1 -1e+60)
                         t_2
                         (if (<= t_1 -5e-153)
                           (*
                            (*
                             (fma (fma 0.0026041666666666665 (* K K) -0.125) (* K K) 1.0)
                             (* J -2.0))
                            (sqrt (+ (pow (* 0.5 (/ U_m J)) 2.0) 1.0)))
                           (if (<= t_1 1e+307) t_2 (* -2.0 (* -0.5 U_m))))))))
                  U_m = fabs(U);
                  double code(double J, double K, double U_m) {
                  	double t_0 = cos((K / 2.0));
                  	double t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_0)), 2.0)));
                  	double t_2 = -2.0 * (J * cos((0.5 * K)));
                  	double tmp;
                  	if (t_1 <= -((double) INFINITY)) {
                  		tmp = -2.0 * (U_m * 0.5);
                  	} else if (t_1 <= -1e+60) {
                  		tmp = t_2;
                  	} else if (t_1 <= -5e-153) {
                  		tmp = (fma(fma(0.0026041666666666665, (K * K), -0.125), (K * K), 1.0) * (J * -2.0)) * sqrt((pow((0.5 * (U_m / J)), 2.0) + 1.0));
                  	} else if (t_1 <= 1e+307) {
                  		tmp = t_2;
                  	} else {
                  		tmp = -2.0 * (-0.5 * U_m);
                  	}
                  	return tmp;
                  }
                  
                  U_m = abs(U)
                  function code(J, K, U_m)
                  	t_0 = cos(Float64(K / 2.0))
                  	t_1 = Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))))
                  	t_2 = Float64(-2.0 * Float64(J * cos(Float64(0.5 * K))))
                  	tmp = 0.0
                  	if (t_1 <= Float64(-Inf))
                  		tmp = Float64(-2.0 * Float64(U_m * 0.5));
                  	elseif (t_1 <= -1e+60)
                  		tmp = t_2;
                  	elseif (t_1 <= -5e-153)
                  		tmp = Float64(Float64(fma(fma(0.0026041666666666665, Float64(K * K), -0.125), Float64(K * K), 1.0) * Float64(J * -2.0)) * sqrt(Float64((Float64(0.5 * Float64(U_m / J)) ^ 2.0) + 1.0)));
                  	elseif (t_1 <= 1e+307)
                  		tmp = t_2;
                  	else
                  		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
                  	end
                  	return tmp
                  end
                  
                  U_m = N[Abs[U], $MachinePrecision]
                  code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[(-2.0 * N[(J * N[Cos[N[(0.5 * K), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$1, (-Infinity)], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$1, -1e+60], t$95$2, If[LessEqual[t$95$1, -5e-153], N[(N[(N[(N[(0.0026041666666666665 * N[(K * K), $MachinePrecision] + -0.125), $MachinePrecision] * N[(K * K), $MachinePrecision] + 1.0), $MachinePrecision] * N[(J * -2.0), $MachinePrecision]), $MachinePrecision] * N[Sqrt[N[(N[Power[N[(0.5 * N[(U$95$m / J), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + 1.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$1, 1e+307], t$95$2, N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]]]]
                  
                  \begin{array}{l}
                  U_m = \left|U\right|
                  
                  \\
                  \begin{array}{l}
                  t_0 := \cos \left(\frac{K}{2}\right)\\
                  t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\
                  t_2 := -2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right)\\
                  \mathbf{if}\;t\_1 \leq -\infty:\\
                  \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\
                  
                  \mathbf{elif}\;t\_1 \leq -1 \cdot 10^{+60}:\\
                  \;\;\;\;t\_2\\
                  
                  \mathbf{elif}\;t\_1 \leq -5 \cdot 10^{-153}:\\
                  \;\;\;\;\left(\mathsf{fma}\left(\mathsf{fma}\left(0.0026041666666666665, K \cdot K, -0.125\right), K \cdot K, 1\right) \cdot \left(J \cdot -2\right)\right) \cdot \sqrt{{\left(0.5 \cdot \frac{U\_m}{J}\right)}^{2} + 1}\\
                  
                  \mathbf{elif}\;t\_1 \leq 10^{+307}:\\
                  \;\;\;\;t\_2\\
                  
                  \mathbf{else}:\\
                  \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
                  
                  
                  \end{array}
                  \end{array}
                  
                  Derivation
                  1. Split input into 4 regimes
                  2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0

                    1. Initial program 73.3%

                      \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                    2. Taylor expanded in J around 0

                      \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                    3. Step-by-step derivation
                      1. lower-*.f64N/A

                        \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                      2. lower-*.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                      3. lower-cos.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                      4. lower-*.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      5. lower-sqrt.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      6. lower-*.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      7. lower-/.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      8. lower-pow.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      9. lower-pow.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      10. lower-cos.f64N/A

                        \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                      11. lower-*.f6414.8

                        \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                    4. Applied rewrites14.8%

                      \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                    5. Taylor expanded in U around 0

                      \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
                    6. Step-by-step derivation
                      1. lower-*.f64N/A

                        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
                      2. lower-*.f64N/A

                        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                      3. lower-cos.f64N/A

                        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                      4. lower-*.f64N/A

                        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                      5. lower-sqrt.f64N/A

                        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                      6. lower-/.f64N/A

                        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                      7. lower-pow.f64N/A

                        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                      8. lower-cos.f64N/A

                        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                      9. lower-*.f6425.6

                        \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
                    7. Applied rewrites25.6%

                      \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
                    8. Taylor expanded in K around 0

                      \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
                    9. Step-by-step derivation
                      1. Applied rewrites26.4%

                        \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

                      if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -9.9999999999999995e59 or -5.00000000000000033e-153 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < 9.99999999999999986e306

                      1. Initial program 73.3%

                        \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                      2. Taylor expanded in J around 0

                        \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                      3. Step-by-step derivation
                        1. lower-*.f64N/A

                          \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                        2. lower-*.f64N/A

                          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                        3. lower-cos.f64N/A

                          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                        4. lower-*.f64N/A

                          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                        5. lower-sqrt.f64N/A

                          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                        6. lower-*.f64N/A

                          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                        7. lower-/.f64N/A

                          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                        8. lower-pow.f64N/A

                          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                        9. lower-pow.f64N/A

                          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                        10. lower-cos.f64N/A

                          \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                        11. lower-*.f6414.8

                          \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                      4. Applied rewrites14.8%

                        \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                      5. Taylor expanded in K around 0

                        \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                      6. Step-by-step derivation
                        1. lower-sqrt.f64N/A

                          \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                        2. lower-*.f64N/A

                          \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                        3. lower-pow.f6414.9

                          \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                      7. Applied rewrites14.9%

                        \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                      8. Taylor expanded in U around -inf

                        \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                      9. Step-by-step derivation
                        1. lower-*.f6426.5

                          \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                      10. Applied rewrites26.5%

                        \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                      11. Taylor expanded in J around inf

                        \[\leadsto \color{blue}{-2 \cdot \left(J \cdot \cos \left(\frac{1}{2} \cdot K\right)\right)} \]
                      12. Step-by-step derivation
                        1. lower-*.f64N/A

                          \[\leadsto -2 \cdot \color{blue}{\left(J \cdot \cos \left(\frac{1}{2} \cdot K\right)\right)} \]
                        2. lower-*.f64N/A

                          \[\leadsto -2 \cdot \left(J \cdot \color{blue}{\cos \left(\frac{1}{2} \cdot K\right)}\right) \]
                        3. lower-cos.f64N/A

                          \[\leadsto -2 \cdot \left(J \cdot \cos \left(\frac{1}{2} \cdot K\right)\right) \]
                        4. lower-*.f6452.4

                          \[\leadsto -2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right) \]
                      13. Applied rewrites52.4%

                        \[\leadsto \color{blue}{-2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right)} \]

                      if -9.9999999999999995e59 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -5.00000000000000033e-153

                      1. Initial program 73.3%

                        \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                      2. Taylor expanded in K around 0

                        \[\leadsto \left(\left(-2 \cdot J\right) \cdot \color{blue}{\left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                      3. Step-by-step derivation
                        1. lower-+.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + \color{blue}{{K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                        2. lower-*.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \color{blue}{\left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                        3. lower-pow.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\color{blue}{\frac{1}{384} \cdot {K}^{2}} - \frac{1}{8}\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                        4. lower--.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \color{blue}{\frac{1}{8}}\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                        5. lower-*.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                        6. lower-pow.f6438.2

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(0.0026041666666666665 \cdot {K}^{2} - 0.125\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                      4. Applied rewrites38.2%

                        \[\leadsto \left(\left(-2 \cdot J\right) \cdot \color{blue}{\left(1 + {K}^{2} \cdot \left(0.0026041666666666665 \cdot {K}^{2} - 0.125\right)\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                      5. Taylor expanded in K around 0

                        \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \color{blue}{\left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)}}\right)}^{2}} \]
                      6. Step-by-step derivation
                        1. lower-+.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \left(1 + \color{blue}{{K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)}\right)}\right)}^{2}} \]
                        2. lower-*.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \color{blue}{\left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)}\right)}\right)}^{2}} \]
                        3. lower-pow.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\color{blue}{\frac{1}{384} \cdot {K}^{2}} - \frac{1}{8}\right)\right)}\right)}^{2}} \]
                        4. lower--.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \color{blue}{\frac{1}{8}}\right)\right)}\right)}^{2}} \]
                        5. lower-*.f64N/A

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(\frac{1}{384} \cdot {K}^{2} - \frac{1}{8}\right)\right)}\right)}^{2}} \]
                        6. lower-pow.f6439.1

                          \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(0.0026041666666666665 \cdot {K}^{2} - 0.125\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(0.0026041666666666665 \cdot {K}^{2} - 0.125\right)\right)}\right)}^{2}} \]
                      7. Applied rewrites39.1%

                        \[\leadsto \left(\left(-2 \cdot J\right) \cdot \left(1 + {K}^{2} \cdot \left(0.0026041666666666665 \cdot {K}^{2} - 0.125\right)\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \color{blue}{\left(1 + {K}^{2} \cdot \left(0.0026041666666666665 \cdot {K}^{2} - 0.125\right)\right)}}\right)}^{2}} \]
                      8. Step-by-step derivation
                        1. Applied rewrites39.1%

                          \[\leadsto \color{blue}{\left(\mathsf{fma}\left(\mathsf{fma}\left(0.0026041666666666665, K \cdot K, -0.125\right), K \cdot K, 1\right) \cdot \left(J \cdot -2\right)\right) \cdot \sqrt{{\left(\frac{U}{\left(J + J\right) \cdot \mathsf{fma}\left(\mathsf{fma}\left(0.0026041666666666665, K \cdot K, -0.125\right), K \cdot K, 1\right)}\right)}^{2} + 1}} \]
                        2. Taylor expanded in K around 0

                          \[\leadsto \left(\mathsf{fma}\left(\mathsf{fma}\left(\frac{1}{384}, K \cdot K, \frac{-1}{8}\right), K \cdot K, 1\right) \cdot \left(J \cdot -2\right)\right) \cdot \sqrt{{\color{blue}{\left(\frac{1}{2} \cdot \frac{U}{J}\right)}}^{2} + 1} \]
                        3. Step-by-step derivation
                          1. lower-*.f64N/A

                            \[\leadsto \left(\mathsf{fma}\left(\mathsf{fma}\left(\frac{1}{384}, K \cdot K, \frac{-1}{8}\right), K \cdot K, 1\right) \cdot \left(J \cdot -2\right)\right) \cdot \sqrt{{\left(\frac{1}{2} \cdot \color{blue}{\frac{U}{J}}\right)}^{2} + 1} \]
                          2. lower-/.f6438.1

                            \[\leadsto \left(\mathsf{fma}\left(\mathsf{fma}\left(0.0026041666666666665, K \cdot K, -0.125\right), K \cdot K, 1\right) \cdot \left(J \cdot -2\right)\right) \cdot \sqrt{{\left(0.5 \cdot \frac{U}{\color{blue}{J}}\right)}^{2} + 1} \]
                        4. Applied rewrites38.1%

                          \[\leadsto \left(\mathsf{fma}\left(\mathsf{fma}\left(0.0026041666666666665, K \cdot K, -0.125\right), K \cdot K, 1\right) \cdot \left(J \cdot -2\right)\right) \cdot \sqrt{{\color{blue}{\left(0.5 \cdot \frac{U}{J}\right)}}^{2} + 1} \]

                        if 9.99999999999999986e306 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

                        1. Initial program 73.3%

                          \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                        2. Taylor expanded in J around 0

                          \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                        3. Step-by-step derivation
                          1. lower-*.f64N/A

                            \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                          2. lower-*.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                          3. lower-cos.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                          4. lower-*.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          5. lower-sqrt.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          6. lower-*.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          7. lower-/.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          8. lower-pow.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          9. lower-pow.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          10. lower-cos.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          11. lower-*.f6414.8

                            \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                        4. Applied rewrites14.8%

                          \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                        5. Taylor expanded in K around 0

                          \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                        6. Step-by-step derivation
                          1. lower-sqrt.f64N/A

                            \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                          2. lower-*.f64N/A

                            \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                          3. lower-pow.f6414.9

                            \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                        7. Applied rewrites14.9%

                          \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                        8. Taylor expanded in U around -inf

                          \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                        9. Step-by-step derivation
                          1. lower-*.f6426.5

                            \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                        10. Applied rewrites26.5%

                          \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                      9. Recombined 4 regimes into one program.
                      10. Add Preprocessing

                      Alternative 9: 77.6% accurate, 0.4× speedup?

                      \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\ \mathbf{if}\;t\_1 \leq -\infty:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{elif}\;t\_1 \leq 10^{+307}:\\ \;\;\;\;-2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right)\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
                      U_m = (fabs.f64 U)
                      (FPCore (J K U_m)
                       :precision binary64
                       (let* ((t_0 (cos (/ K 2.0)))
                              (t_1
                               (*
                                (* (* -2.0 J) t_0)
                                (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_0)) 2.0))))))
                         (if (<= t_1 (- INFINITY))
                           (* -2.0 (* U_m 0.5))
                           (if (<= t_1 1e+307)
                             (* -2.0 (* J (cos (* 0.5 K))))
                             (* -2.0 (* -0.5 U_m))))))
                      U_m = fabs(U);
                      double code(double J, double K, double U_m) {
                      	double t_0 = cos((K / 2.0));
                      	double t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_0)), 2.0)));
                      	double tmp;
                      	if (t_1 <= -((double) INFINITY)) {
                      		tmp = -2.0 * (U_m * 0.5);
                      	} else if (t_1 <= 1e+307) {
                      		tmp = -2.0 * (J * cos((0.5 * K)));
                      	} else {
                      		tmp = -2.0 * (-0.5 * U_m);
                      	}
                      	return tmp;
                      }
                      
                      U_m = Math.abs(U);
                      public static double code(double J, double K, double U_m) {
                      	double t_0 = Math.cos((K / 2.0));
                      	double t_1 = ((-2.0 * J) * t_0) * Math.sqrt((1.0 + Math.pow((U_m / ((2.0 * J) * t_0)), 2.0)));
                      	double tmp;
                      	if (t_1 <= -Double.POSITIVE_INFINITY) {
                      		tmp = -2.0 * (U_m * 0.5);
                      	} else if (t_1 <= 1e+307) {
                      		tmp = -2.0 * (J * Math.cos((0.5 * K)));
                      	} else {
                      		tmp = -2.0 * (-0.5 * U_m);
                      	}
                      	return tmp;
                      }
                      
                      U_m = math.fabs(U)
                      def code(J, K, U_m):
                      	t_0 = math.cos((K / 2.0))
                      	t_1 = ((-2.0 * J) * t_0) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_0)), 2.0)))
                      	tmp = 0
                      	if t_1 <= -math.inf:
                      		tmp = -2.0 * (U_m * 0.5)
                      	elif t_1 <= 1e+307:
                      		tmp = -2.0 * (J * math.cos((0.5 * K)))
                      	else:
                      		tmp = -2.0 * (-0.5 * U_m)
                      	return tmp
                      
                      U_m = abs(U)
                      function code(J, K, U_m)
                      	t_0 = cos(Float64(K / 2.0))
                      	t_1 = Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_0)) ^ 2.0))))
                      	tmp = 0.0
                      	if (t_1 <= Float64(-Inf))
                      		tmp = Float64(-2.0 * Float64(U_m * 0.5));
                      	elseif (t_1 <= 1e+307)
                      		tmp = Float64(-2.0 * Float64(J * cos(Float64(0.5 * K))));
                      	else
                      		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
                      	end
                      	return tmp
                      end
                      
                      U_m = abs(U);
                      function tmp_2 = code(J, K, U_m)
                      	t_0 = cos((K / 2.0));
                      	t_1 = ((-2.0 * J) * t_0) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_0)) ^ 2.0)));
                      	tmp = 0.0;
                      	if (t_1 <= -Inf)
                      		tmp = -2.0 * (U_m * 0.5);
                      	elseif (t_1 <= 1e+307)
                      		tmp = -2.0 * (J * cos((0.5 * K)));
                      	else
                      		tmp = -2.0 * (-0.5 * U_m);
                      	end
                      	tmp_2 = tmp;
                      end
                      
                      U_m = N[Abs[U], $MachinePrecision]
                      code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$1, (-Infinity)], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$1, 1e+307], N[(-2.0 * N[(J * N[Cos[N[(0.5 * K), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]
                      
                      \begin{array}{l}
                      U_m = \left|U\right|
                      
                      \\
                      \begin{array}{l}
                      t_0 := \cos \left(\frac{K}{2}\right)\\
                      t_1 := \left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}}\\
                      \mathbf{if}\;t\_1 \leq -\infty:\\
                      \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\
                      
                      \mathbf{elif}\;t\_1 \leq 10^{+307}:\\
                      \;\;\;\;-2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right)\\
                      
                      \mathbf{else}:\\
                      \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
                      
                      
                      \end{array}
                      \end{array}
                      
                      Derivation
                      1. Split input into 3 regimes
                      2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0

                        1. Initial program 73.3%

                          \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                        2. Taylor expanded in J around 0

                          \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                        3. Step-by-step derivation
                          1. lower-*.f64N/A

                            \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                          2. lower-*.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                          3. lower-cos.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                          4. lower-*.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          5. lower-sqrt.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          6. lower-*.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          7. lower-/.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          8. lower-pow.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          9. lower-pow.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          10. lower-cos.f64N/A

                            \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                          11. lower-*.f6414.8

                            \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                        4. Applied rewrites14.8%

                          \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                        5. Taylor expanded in U around 0

                          \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
                        6. Step-by-step derivation
                          1. lower-*.f64N/A

                            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
                          2. lower-*.f64N/A

                            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                          3. lower-cos.f64N/A

                            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                          4. lower-*.f64N/A

                            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                          5. lower-sqrt.f64N/A

                            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                          6. lower-/.f64N/A

                            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                          7. lower-pow.f64N/A

                            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                          8. lower-cos.f64N/A

                            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                          9. lower-*.f6425.6

                            \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
                        7. Applied rewrites25.6%

                          \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
                        8. Taylor expanded in K around 0

                          \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
                        9. Step-by-step derivation
                          1. Applied rewrites26.4%

                            \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

                          if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < 9.99999999999999986e306

                          1. Initial program 73.3%

                            \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                          2. Taylor expanded in J around 0

                            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                          3. Step-by-step derivation
                            1. lower-*.f64N/A

                              \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                            2. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                            3. lower-cos.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                            4. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            5. lower-sqrt.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            6. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            7. lower-/.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            8. lower-pow.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            9. lower-pow.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            10. lower-cos.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            11. lower-*.f6414.8

                              \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                          4. Applied rewrites14.8%

                            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                          5. Taylor expanded in K around 0

                            \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                          6. Step-by-step derivation
                            1. lower-sqrt.f64N/A

                              \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                            2. lower-*.f64N/A

                              \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                            3. lower-pow.f6414.9

                              \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                          7. Applied rewrites14.9%

                            \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                          8. Taylor expanded in U around -inf

                            \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                          9. Step-by-step derivation
                            1. lower-*.f6426.5

                              \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                          10. Applied rewrites26.5%

                            \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                          11. Taylor expanded in J around inf

                            \[\leadsto \color{blue}{-2 \cdot \left(J \cdot \cos \left(\frac{1}{2} \cdot K\right)\right)} \]
                          12. Step-by-step derivation
                            1. lower-*.f64N/A

                              \[\leadsto -2 \cdot \color{blue}{\left(J \cdot \cos \left(\frac{1}{2} \cdot K\right)\right)} \]
                            2. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(J \cdot \color{blue}{\cos \left(\frac{1}{2} \cdot K\right)}\right) \]
                            3. lower-cos.f64N/A

                              \[\leadsto -2 \cdot \left(J \cdot \cos \left(\frac{1}{2} \cdot K\right)\right) \]
                            4. lower-*.f6452.4

                              \[\leadsto -2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right) \]
                          13. Applied rewrites52.4%

                            \[\leadsto \color{blue}{-2 \cdot \left(J \cdot \cos \left(0.5 \cdot K\right)\right)} \]

                          if 9.99999999999999986e306 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

                          1. Initial program 73.3%

                            \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                          2. Taylor expanded in J around 0

                            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                          3. Step-by-step derivation
                            1. lower-*.f64N/A

                              \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                            2. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                            3. lower-cos.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                            4. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            5. lower-sqrt.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            6. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            7. lower-/.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            8. lower-pow.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            9. lower-pow.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            10. lower-cos.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            11. lower-*.f6414.8

                              \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                          4. Applied rewrites14.8%

                            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                          5. Taylor expanded in K around 0

                            \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                          6. Step-by-step derivation
                            1. lower-sqrt.f64N/A

                              \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                            2. lower-*.f64N/A

                              \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                            3. lower-pow.f6414.9

                              \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                          7. Applied rewrites14.9%

                            \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                          8. Taylor expanded in U around -inf

                            \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                          9. Step-by-step derivation
                            1. lower-*.f6426.5

                              \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                          10. Applied rewrites26.5%

                            \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                        10. Recombined 3 regimes into one program.
                        11. Add Preprocessing

                        Alternative 10: 54.3% accurate, 0.3× speedup?

                        \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := -2 \cdot \left(U\_m \cdot 0.5\right)\\ t_1 := \cos \left(\frac{K}{2}\right)\\ t_2 := \left(\left(-2 \cdot J\right) \cdot t\_1\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_1}\right)}^{2}}\\ \mathbf{if}\;t\_2 \leq -\infty:\\ \;\;\;\;t\_0\\ \mathbf{elif}\;t\_2 \leq -2 \cdot 10^{-29}:\\ \;\;\;\;\left(-2 \cdot J\right) \cdot 1\\ \mathbf{elif}\;t\_2 \leq -1 \cdot 10^{-229}:\\ \;\;\;\;t\_0\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
                        U_m = (fabs.f64 U)
                        (FPCore (J K U_m)
                         :precision binary64
                         (let* ((t_0 (* -2.0 (* U_m 0.5)))
                                (t_1 (cos (/ K 2.0)))
                                (t_2
                                 (*
                                  (* (* -2.0 J) t_1)
                                  (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_1)) 2.0))))))
                           (if (<= t_2 (- INFINITY))
                             t_0
                             (if (<= t_2 -2e-29)
                               (* (* -2.0 J) 1.0)
                               (if (<= t_2 -1e-229) t_0 (* -2.0 (* -0.5 U_m)))))))
                        U_m = fabs(U);
                        double code(double J, double K, double U_m) {
                        	double t_0 = -2.0 * (U_m * 0.5);
                        	double t_1 = cos((K / 2.0));
                        	double t_2 = ((-2.0 * J) * t_1) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_1)), 2.0)));
                        	double tmp;
                        	if (t_2 <= -((double) INFINITY)) {
                        		tmp = t_0;
                        	} else if (t_2 <= -2e-29) {
                        		tmp = (-2.0 * J) * 1.0;
                        	} else if (t_2 <= -1e-229) {
                        		tmp = t_0;
                        	} else {
                        		tmp = -2.0 * (-0.5 * U_m);
                        	}
                        	return tmp;
                        }
                        
                        U_m = Math.abs(U);
                        public static double code(double J, double K, double U_m) {
                        	double t_0 = -2.0 * (U_m * 0.5);
                        	double t_1 = Math.cos((K / 2.0));
                        	double t_2 = ((-2.0 * J) * t_1) * Math.sqrt((1.0 + Math.pow((U_m / ((2.0 * J) * t_1)), 2.0)));
                        	double tmp;
                        	if (t_2 <= -Double.POSITIVE_INFINITY) {
                        		tmp = t_0;
                        	} else if (t_2 <= -2e-29) {
                        		tmp = (-2.0 * J) * 1.0;
                        	} else if (t_2 <= -1e-229) {
                        		tmp = t_0;
                        	} else {
                        		tmp = -2.0 * (-0.5 * U_m);
                        	}
                        	return tmp;
                        }
                        
                        U_m = math.fabs(U)
                        def code(J, K, U_m):
                        	t_0 = -2.0 * (U_m * 0.5)
                        	t_1 = math.cos((K / 2.0))
                        	t_2 = ((-2.0 * J) * t_1) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_1)), 2.0)))
                        	tmp = 0
                        	if t_2 <= -math.inf:
                        		tmp = t_0
                        	elif t_2 <= -2e-29:
                        		tmp = (-2.0 * J) * 1.0
                        	elif t_2 <= -1e-229:
                        		tmp = t_0
                        	else:
                        		tmp = -2.0 * (-0.5 * U_m)
                        	return tmp
                        
                        U_m = abs(U)
                        function code(J, K, U_m)
                        	t_0 = Float64(-2.0 * Float64(U_m * 0.5))
                        	t_1 = cos(Float64(K / 2.0))
                        	t_2 = Float64(Float64(Float64(-2.0 * J) * t_1) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_1)) ^ 2.0))))
                        	tmp = 0.0
                        	if (t_2 <= Float64(-Inf))
                        		tmp = t_0;
                        	elseif (t_2 <= -2e-29)
                        		tmp = Float64(Float64(-2.0 * J) * 1.0);
                        	elseif (t_2 <= -1e-229)
                        		tmp = t_0;
                        	else
                        		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
                        	end
                        	return tmp
                        end
                        
                        U_m = abs(U);
                        function tmp_2 = code(J, K, U_m)
                        	t_0 = -2.0 * (U_m * 0.5);
                        	t_1 = cos((K / 2.0));
                        	t_2 = ((-2.0 * J) * t_1) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_1)) ^ 2.0)));
                        	tmp = 0.0;
                        	if (t_2 <= -Inf)
                        		tmp = t_0;
                        	elseif (t_2 <= -2e-29)
                        		tmp = (-2.0 * J) * 1.0;
                        	elseif (t_2 <= -1e-229)
                        		tmp = t_0;
                        	else
                        		tmp = -2.0 * (-0.5 * U_m);
                        	end
                        	tmp_2 = tmp;
                        end
                        
                        U_m = N[Abs[U], $MachinePrecision]
                        code[J_, K_, U$95$m_] := Block[{t$95$0 = N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$1), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$1), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$2, (-Infinity)], t$95$0, If[LessEqual[t$95$2, -2e-29], N[(N[(-2.0 * J), $MachinePrecision] * 1.0), $MachinePrecision], If[LessEqual[t$95$2, -1e-229], t$95$0, N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]]]]]
                        
                        \begin{array}{l}
                        U_m = \left|U\right|
                        
                        \\
                        \begin{array}{l}
                        t_0 := -2 \cdot \left(U\_m \cdot 0.5\right)\\
                        t_1 := \cos \left(\frac{K}{2}\right)\\
                        t_2 := \left(\left(-2 \cdot J\right) \cdot t\_1\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_1}\right)}^{2}}\\
                        \mathbf{if}\;t\_2 \leq -\infty:\\
                        \;\;\;\;t\_0\\
                        
                        \mathbf{elif}\;t\_2 \leq -2 \cdot 10^{-29}:\\
                        \;\;\;\;\left(-2 \cdot J\right) \cdot 1\\
                        
                        \mathbf{elif}\;t\_2 \leq -1 \cdot 10^{-229}:\\
                        \;\;\;\;t\_0\\
                        
                        \mathbf{else}:\\
                        \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
                        
                        
                        \end{array}
                        \end{array}
                        
                        Derivation
                        1. Split input into 3 regimes
                        2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -inf.0 or -1.99999999999999989e-29 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -1.00000000000000007e-229

                          1. Initial program 73.3%

                            \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                          2. Taylor expanded in J around 0

                            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                          3. Step-by-step derivation
                            1. lower-*.f64N/A

                              \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                            2. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                            3. lower-cos.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                            4. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            5. lower-sqrt.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            6. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            7. lower-/.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            8. lower-pow.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            9. lower-pow.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            10. lower-cos.f64N/A

                              \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                            11. lower-*.f6414.8

                              \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                          4. Applied rewrites14.8%

                            \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                          5. Taylor expanded in U around 0

                            \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
                          6. Step-by-step derivation
                            1. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
                            2. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                            3. lower-cos.f64N/A

                              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                            4. lower-*.f64N/A

                              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                            5. lower-sqrt.f64N/A

                              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                            6. lower-/.f64N/A

                              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                            7. lower-pow.f64N/A

                              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                            8. lower-cos.f64N/A

                              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                            9. lower-*.f6425.6

                              \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
                          7. Applied rewrites25.6%

                            \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
                          8. Taylor expanded in K around 0

                            \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
                          9. Step-by-step derivation
                            1. Applied rewrites26.4%

                              \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

                            if -inf.0 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -1.99999999999999989e-29

                            1. Initial program 73.3%

                              \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                            2. Step-by-step derivation
                              1. lift-*.f64N/A

                                \[\leadsto \color{blue}{\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              2. *-commutativeN/A

                                \[\leadsto \color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot \left(-2 \cdot J\right)\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              3. lift-*.f64N/A

                                \[\leadsto \left(\cos \left(\frac{K}{2}\right) \cdot \color{blue}{\left(-2 \cdot J\right)}\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              4. associate-*r*N/A

                                \[\leadsto \color{blue}{\left(\left(\cos \left(\frac{K}{2}\right) \cdot -2\right) \cdot J\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              5. lower-*.f64N/A

                                \[\leadsto \color{blue}{\left(\left(\cos \left(\frac{K}{2}\right) \cdot -2\right) \cdot J\right)} \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              6. lower-*.f6473.4

                                \[\leadsto \left(\color{blue}{\left(\cos \left(\frac{K}{2}\right) \cdot -2\right)} \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              7. lift-cos.f64N/A

                                \[\leadsto \left(\left(\color{blue}{\cos \left(\frac{K}{2}\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              8. cos-neg-revN/A

                                \[\leadsto \left(\left(\color{blue}{\cos \left(\mathsf{neg}\left(\frac{K}{2}\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              9. lower-cos.f64N/A

                                \[\leadsto \left(\left(\color{blue}{\cos \left(\mathsf{neg}\left(\frac{K}{2}\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              10. lift-/.f64N/A

                                \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(\color{blue}{\frac{K}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              11. mult-flipN/A

                                \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(\color{blue}{K \cdot \frac{1}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              12. metadata-evalN/A

                                \[\leadsto \left(\left(\cos \left(\mathsf{neg}\left(K \cdot \color{blue}{\frac{1}{2}}\right)\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              13. distribute-rgt-neg-inN/A

                                \[\leadsto \left(\left(\cos \color{blue}{\left(K \cdot \left(\mathsf{neg}\left(\frac{1}{2}\right)\right)\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              14. metadata-evalN/A

                                \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{\frac{-1}{2}}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              15. metadata-evalN/A

                                \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{\frac{1}{-2}}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              16. lower-*.f64N/A

                                \[\leadsto \left(\left(\cos \color{blue}{\left(K \cdot \frac{1}{-2}\right)} \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              17. metadata-eval73.4

                                \[\leadsto \left(\left(\cos \left(K \cdot \color{blue}{-0.5}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                              18. lift-sqrt.f64N/A

                                \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \color{blue}{\sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
                              19. lift-+.f64N/A

                                \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \sqrt{\color{blue}{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}}} \]
                            3. Applied rewrites84.8%

                              \[\leadsto \color{blue}{\left(\left(\cos \left(K \cdot -0.5\right) \cdot -2\right) \cdot J\right) \cdot \cosh \sinh^{-1} \left(\frac{U}{\left(J + J\right) \cdot \cos \left(K \cdot -0.5\right)}\right)} \]
                            4. Taylor expanded in J around inf

                              \[\leadsto \left(\left(\cos \left(K \cdot \frac{-1}{2}\right) \cdot -2\right) \cdot J\right) \cdot \color{blue}{1} \]
                            5. Step-by-step derivation
                              1. Applied rewrites52.4%

                                \[\leadsto \left(\left(\cos \left(K \cdot -0.5\right) \cdot -2\right) \cdot J\right) \cdot \color{blue}{1} \]
                              2. Taylor expanded in K around 0

                                \[\leadsto \left(\color{blue}{-2} \cdot J\right) \cdot 1 \]
                              3. Step-by-step derivation
                                1. Applied rewrites29.4%

                                  \[\leadsto \left(\color{blue}{-2} \cdot J\right) \cdot 1 \]

                                if -1.00000000000000007e-229 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

                                1. Initial program 73.3%

                                  \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                                2. Taylor expanded in J around 0

                                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                                3. Step-by-step derivation
                                  1. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                                  2. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                                  3. lower-cos.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                                  4. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  5. lower-sqrt.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  6. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  7. lower-/.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  8. lower-pow.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  9. lower-pow.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  10. lower-cos.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  11. lower-*.f6414.8

                                    \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                                4. Applied rewrites14.8%

                                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                                5. Taylor expanded in K around 0

                                  \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                                6. Step-by-step derivation
                                  1. lower-sqrt.f64N/A

                                    \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                                  2. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                                  3. lower-pow.f6414.9

                                    \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                                7. Applied rewrites14.9%

                                  \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                                8. Taylor expanded in U around -inf

                                  \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                                9. Step-by-step derivation
                                  1. lower-*.f6426.5

                                    \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                                10. Applied rewrites26.5%

                                  \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                              4. Recombined 3 regimes into one program.
                              5. Add Preprocessing

                              Alternative 11: 51.1% accurate, 0.9× speedup?

                              \[\begin{array}{l} U_m = \left|U\right| \\ \begin{array}{l} t_0 := \cos \left(\frac{K}{2}\right)\\ \mathbf{if}\;\left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}} \leq -1 \cdot 10^{-229}:\\ \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\ \mathbf{else}:\\ \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\ \end{array} \end{array} \]
                              U_m = (fabs.f64 U)
                              (FPCore (J K U_m)
                               :precision binary64
                               (let* ((t_0 (cos (/ K 2.0))))
                                 (if (<=
                                      (*
                                       (* (* -2.0 J) t_0)
                                       (sqrt (+ 1.0 (pow (/ U_m (* (* 2.0 J) t_0)) 2.0))))
                                      -1e-229)
                                   (* -2.0 (* U_m 0.5))
                                   (* -2.0 (* -0.5 U_m)))))
                              U_m = fabs(U);
                              double code(double J, double K, double U_m) {
                              	double t_0 = cos((K / 2.0));
                              	double tmp;
                              	if ((((-2.0 * J) * t_0) * sqrt((1.0 + pow((U_m / ((2.0 * J) * t_0)), 2.0)))) <= -1e-229) {
                              		tmp = -2.0 * (U_m * 0.5);
                              	} else {
                              		tmp = -2.0 * (-0.5 * U_m);
                              	}
                              	return tmp;
                              }
                              
                              U_m =     private
                              module fmin_fmax_functions
                                  implicit none
                                  private
                                  public fmax
                                  public fmin
                              
                                  interface fmax
                                      module procedure fmax88
                                      module procedure fmax44
                                      module procedure fmax84
                                      module procedure fmax48
                                  end interface
                                  interface fmin
                                      module procedure fmin88
                                      module procedure fmin44
                                      module procedure fmin84
                                      module procedure fmin48
                                  end interface
                              contains
                                  real(8) function fmax88(x, y) result (res)
                                      real(8), intent (in) :: x
                                      real(8), intent (in) :: y
                                      res = merge(y, merge(x, max(x, y), y /= y), x /= x)
                                  end function
                                  real(4) function fmax44(x, y) result (res)
                                      real(4), intent (in) :: x
                                      real(4), intent (in) :: y
                                      res = merge(y, merge(x, max(x, y), y /= y), x /= x)
                                  end function
                                  real(8) function fmax84(x, y) result(res)
                                      real(8), intent (in) :: x
                                      real(4), intent (in) :: y
                                      res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
                                  end function
                                  real(8) function fmax48(x, y) result(res)
                                      real(4), intent (in) :: x
                                      real(8), intent (in) :: y
                                      res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
                                  end function
                                  real(8) function fmin88(x, y) result (res)
                                      real(8), intent (in) :: x
                                      real(8), intent (in) :: y
                                      res = merge(y, merge(x, min(x, y), y /= y), x /= x)
                                  end function
                                  real(4) function fmin44(x, y) result (res)
                                      real(4), intent (in) :: x
                                      real(4), intent (in) :: y
                                      res = merge(y, merge(x, min(x, y), y /= y), x /= x)
                                  end function
                                  real(8) function fmin84(x, y) result(res)
                                      real(8), intent (in) :: x
                                      real(4), intent (in) :: y
                                      res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
                                  end function
                                  real(8) function fmin48(x, y) result(res)
                                      real(4), intent (in) :: x
                                      real(8), intent (in) :: y
                                      res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
                                  end function
                              end module
                              
                              real(8) function code(j, k, u_m)
                              use fmin_fmax_functions
                                  real(8), intent (in) :: j
                                  real(8), intent (in) :: k
                                  real(8), intent (in) :: u_m
                                  real(8) :: t_0
                                  real(8) :: tmp
                                  t_0 = cos((k / 2.0d0))
                                  if (((((-2.0d0) * j) * t_0) * sqrt((1.0d0 + ((u_m / ((2.0d0 * j) * t_0)) ** 2.0d0)))) <= (-1d-229)) then
                                      tmp = (-2.0d0) * (u_m * 0.5d0)
                                  else
                                      tmp = (-2.0d0) * ((-0.5d0) * u_m)
                                  end if
                                  code = tmp
                              end function
                              
                              U_m = Math.abs(U);
                              public static double code(double J, double K, double U_m) {
                              	double t_0 = Math.cos((K / 2.0));
                              	double tmp;
                              	if ((((-2.0 * J) * t_0) * Math.sqrt((1.0 + Math.pow((U_m / ((2.0 * J) * t_0)), 2.0)))) <= -1e-229) {
                              		tmp = -2.0 * (U_m * 0.5);
                              	} else {
                              		tmp = -2.0 * (-0.5 * U_m);
                              	}
                              	return tmp;
                              }
                              
                              U_m = math.fabs(U)
                              def code(J, K, U_m):
                              	t_0 = math.cos((K / 2.0))
                              	tmp = 0
                              	if (((-2.0 * J) * t_0) * math.sqrt((1.0 + math.pow((U_m / ((2.0 * J) * t_0)), 2.0)))) <= -1e-229:
                              		tmp = -2.0 * (U_m * 0.5)
                              	else:
                              		tmp = -2.0 * (-0.5 * U_m)
                              	return tmp
                              
                              U_m = abs(U)
                              function code(J, K, U_m)
                              	t_0 = cos(Float64(K / 2.0))
                              	tmp = 0.0
                              	if (Float64(Float64(Float64(-2.0 * J) * t_0) * sqrt(Float64(1.0 + (Float64(U_m / Float64(Float64(2.0 * J) * t_0)) ^ 2.0)))) <= -1e-229)
                              		tmp = Float64(-2.0 * Float64(U_m * 0.5));
                              	else
                              		tmp = Float64(-2.0 * Float64(-0.5 * U_m));
                              	end
                              	return tmp
                              end
                              
                              U_m = abs(U);
                              function tmp_2 = code(J, K, U_m)
                              	t_0 = cos((K / 2.0));
                              	tmp = 0.0;
                              	if ((((-2.0 * J) * t_0) * sqrt((1.0 + ((U_m / ((2.0 * J) * t_0)) ^ 2.0)))) <= -1e-229)
                              		tmp = -2.0 * (U_m * 0.5);
                              	else
                              		tmp = -2.0 * (-0.5 * U_m);
                              	end
                              	tmp_2 = tmp;
                              end
                              
                              U_m = N[Abs[U], $MachinePrecision]
                              code[J_, K_, U$95$m_] := Block[{t$95$0 = N[Cos[N[(K / 2.0), $MachinePrecision]], $MachinePrecision]}, If[LessEqual[N[(N[(N[(-2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision] * N[Sqrt[N[(1.0 + N[Power[N[(U$95$m / N[(N[(2.0 * J), $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], -1e-229], N[(-2.0 * N[(U$95$m * 0.5), $MachinePrecision]), $MachinePrecision], N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]]]
                              
                              \begin{array}{l}
                              U_m = \left|U\right|
                              
                              \\
                              \begin{array}{l}
                              t_0 := \cos \left(\frac{K}{2}\right)\\
                              \mathbf{if}\;\left(\left(-2 \cdot J\right) \cdot t\_0\right) \cdot \sqrt{1 + {\left(\frac{U\_m}{\left(2 \cdot J\right) \cdot t\_0}\right)}^{2}} \leq -1 \cdot 10^{-229}:\\
                              \;\;\;\;-2 \cdot \left(U\_m \cdot 0.5\right)\\
                              
                              \mathbf{else}:\\
                              \;\;\;\;-2 \cdot \left(-0.5 \cdot U\_m\right)\\
                              
                              
                              \end{array}
                              \end{array}
                              
                              Derivation
                              1. Split input into 2 regimes
                              2. if (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64))))) < -1.00000000000000007e-229

                                1. Initial program 73.3%

                                  \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                                2. Taylor expanded in J around 0

                                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                                3. Step-by-step derivation
                                  1. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                                  2. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                                  3. lower-cos.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                                  4. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  5. lower-sqrt.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  6. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  7. lower-/.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  8. lower-pow.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  9. lower-pow.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  10. lower-cos.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  11. lower-*.f6414.8

                                    \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                                4. Applied rewrites14.8%

                                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                                5. Taylor expanded in U around 0

                                  \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)}\right) \]
                                6. Step-by-step derivation
                                  1. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right)\right) \]
                                  2. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                                  3. lower-cos.f64N/A

                                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                                  4. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                                  5. lower-sqrt.f64N/A

                                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                                  6. lower-/.f64N/A

                                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                                  7. lower-pow.f64N/A

                                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                                  8. lower-cos.f64N/A

                                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{\frac{1}{4}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)\right) \]
                                  9. lower-*.f6425.6

                                    \[\leadsto -2 \cdot \left(U \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)\right) \]
                                7. Applied rewrites25.6%

                                  \[\leadsto -2 \cdot \left(U \cdot \color{blue}{\left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{\frac{0.25}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)}\right) \]
                                8. Taylor expanded in K around 0

                                  \[\leadsto -2 \cdot \left(U \cdot \frac{1}{2}\right) \]
                                9. Step-by-step derivation
                                  1. Applied rewrites26.4%

                                    \[\leadsto -2 \cdot \left(U \cdot 0.5\right) \]

                                  if -1.00000000000000007e-229 < (*.f64 (*.f64 (*.f64 #s(literal -2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64)))) (sqrt.f64 (+.f64 #s(literal 1 binary64) (pow.f64 (/.f64 U (*.f64 (*.f64 #s(literal 2 binary64) J) (cos.f64 (/.f64 K #s(literal 2 binary64))))) #s(literal 2 binary64)))))

                                  1. Initial program 73.3%

                                    \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                                  2. Taylor expanded in J around 0

                                    \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                                  3. Step-by-step derivation
                                    1. lower-*.f64N/A

                                      \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                                    2. lower-*.f64N/A

                                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                                    3. lower-cos.f64N/A

                                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                                    4. lower-*.f64N/A

                                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                    5. lower-sqrt.f64N/A

                                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                    6. lower-*.f64N/A

                                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                    7. lower-/.f64N/A

                                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                    8. lower-pow.f64N/A

                                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                    9. lower-pow.f64N/A

                                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                    10. lower-cos.f64N/A

                                      \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                    11. lower-*.f6414.8

                                      \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                                  4. Applied rewrites14.8%

                                    \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                                  5. Taylor expanded in K around 0

                                    \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                                  6. Step-by-step derivation
                                    1. lower-sqrt.f64N/A

                                      \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                                    2. lower-*.f64N/A

                                      \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                                    3. lower-pow.f6414.9

                                      \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                                  7. Applied rewrites14.9%

                                    \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                                  8. Taylor expanded in U around -inf

                                    \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                                  9. Step-by-step derivation
                                    1. lower-*.f6426.5

                                      \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                                  10. Applied rewrites26.5%

                                    \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                                10. Recombined 2 regimes into one program.
                                11. Add Preprocessing

                                Alternative 12: 26.5% accurate, 15.9× speedup?

                                \[\begin{array}{l} U_m = \left|U\right| \\ -2 \cdot \left(-0.5 \cdot U\_m\right) \end{array} \]
                                U_m = (fabs.f64 U)
                                (FPCore (J K U_m) :precision binary64 (* -2.0 (* -0.5 U_m)))
                                U_m = fabs(U);
                                double code(double J, double K, double U_m) {
                                	return -2.0 * (-0.5 * U_m);
                                }
                                
                                U_m =     private
                                module fmin_fmax_functions
                                    implicit none
                                    private
                                    public fmax
                                    public fmin
                                
                                    interface fmax
                                        module procedure fmax88
                                        module procedure fmax44
                                        module procedure fmax84
                                        module procedure fmax48
                                    end interface
                                    interface fmin
                                        module procedure fmin88
                                        module procedure fmin44
                                        module procedure fmin84
                                        module procedure fmin48
                                    end interface
                                contains
                                    real(8) function fmax88(x, y) result (res)
                                        real(8), intent (in) :: x
                                        real(8), intent (in) :: y
                                        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
                                    end function
                                    real(4) function fmax44(x, y) result (res)
                                        real(4), intent (in) :: x
                                        real(4), intent (in) :: y
                                        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
                                    end function
                                    real(8) function fmax84(x, y) result(res)
                                        real(8), intent (in) :: x
                                        real(4), intent (in) :: y
                                        res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
                                    end function
                                    real(8) function fmax48(x, y) result(res)
                                        real(4), intent (in) :: x
                                        real(8), intent (in) :: y
                                        res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
                                    end function
                                    real(8) function fmin88(x, y) result (res)
                                        real(8), intent (in) :: x
                                        real(8), intent (in) :: y
                                        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
                                    end function
                                    real(4) function fmin44(x, y) result (res)
                                        real(4), intent (in) :: x
                                        real(4), intent (in) :: y
                                        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
                                    end function
                                    real(8) function fmin84(x, y) result(res)
                                        real(8), intent (in) :: x
                                        real(4), intent (in) :: y
                                        res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
                                    end function
                                    real(8) function fmin48(x, y) result(res)
                                        real(4), intent (in) :: x
                                        real(8), intent (in) :: y
                                        res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
                                    end function
                                end module
                                
                                real(8) function code(j, k, u_m)
                                use fmin_fmax_functions
                                    real(8), intent (in) :: j
                                    real(8), intent (in) :: k
                                    real(8), intent (in) :: u_m
                                    code = (-2.0d0) * ((-0.5d0) * u_m)
                                end function
                                
                                U_m = Math.abs(U);
                                public static double code(double J, double K, double U_m) {
                                	return -2.0 * (-0.5 * U_m);
                                }
                                
                                U_m = math.fabs(U)
                                def code(J, K, U_m):
                                	return -2.0 * (-0.5 * U_m)
                                
                                U_m = abs(U)
                                function code(J, K, U_m)
                                	return Float64(-2.0 * Float64(-0.5 * U_m))
                                end
                                
                                U_m = abs(U);
                                function tmp = code(J, K, U_m)
                                	tmp = -2.0 * (-0.5 * U_m);
                                end
                                
                                U_m = N[Abs[U], $MachinePrecision]
                                code[J_, K_, U$95$m_] := N[(-2.0 * N[(-0.5 * U$95$m), $MachinePrecision]), $MachinePrecision]
                                
                                \begin{array}{l}
                                U_m = \left|U\right|
                                
                                \\
                                -2 \cdot \left(-0.5 \cdot U\_m\right)
                                \end{array}
                                
                                Derivation
                                1. Initial program 73.3%

                                  \[\left(\left(-2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)\right) \cdot \sqrt{1 + {\left(\frac{U}{\left(2 \cdot J\right) \cdot \cos \left(\frac{K}{2}\right)}\right)}^{2}} \]
                                2. Taylor expanded in J around 0

                                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                                3. Step-by-step derivation
                                  1. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \color{blue}{\left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right)} \]
                                  2. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \color{blue}{\sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                                  3. lower-cos.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}}\right) \]
                                  4. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\color{blue}{\frac{1}{4}} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  5. lower-sqrt.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  6. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  7. lower-/.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  8. lower-pow.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  9. lower-pow.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  10. lower-cos.f64N/A

                                    \[\leadsto -2 \cdot \left(\cos \left(\frac{1}{2} \cdot K\right) \cdot \sqrt{\frac{1}{4} \cdot \frac{{U}^{2}}{{\cos \left(\frac{1}{2} \cdot K\right)}^{2}}}\right) \]
                                  11. lower-*.f6414.8

                                    \[\leadsto -2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right) \]
                                4. Applied rewrites14.8%

                                  \[\leadsto \color{blue}{-2 \cdot \left(\cos \left(0.5 \cdot K\right) \cdot \sqrt{0.25 \cdot \frac{{U}^{2}}{{\cos \left(0.5 \cdot K\right)}^{2}}}\right)} \]
                                5. Taylor expanded in K around 0

                                  \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                                6. Step-by-step derivation
                                  1. lower-sqrt.f64N/A

                                    \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                                  2. lower-*.f64N/A

                                    \[\leadsto -2 \cdot \sqrt{\frac{1}{4} \cdot {U}^{2}} \]
                                  3. lower-pow.f6414.9

                                    \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                                7. Applied rewrites14.9%

                                  \[\leadsto -2 \cdot \sqrt{0.25 \cdot {U}^{2}} \]
                                8. Taylor expanded in U around -inf

                                  \[\leadsto -2 \cdot \left(\frac{-1}{2} \cdot U\right) \]
                                9. Step-by-step derivation
                                  1. lower-*.f6426.5

                                    \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                                10. Applied rewrites26.5%

                                  \[\leadsto -2 \cdot \left(-0.5 \cdot U\right) \]
                                11. Add Preprocessing

                                Reproduce

                                ?
                                herbie shell --seed 2025150 
                                (FPCore (J K U)
                                  :name "Maksimov and Kolovsky, Equation (3)"
                                  :precision binary64
                                  (* (* (* -2.0 J) (cos (/ K 2.0))) (sqrt (+ 1.0 (pow (/ U (* (* 2.0 J) (cos (/ K 2.0)))) 2.0)))))