Migdal et al, Equation (64)

Percentage Accurate: 99.5% → 99.6%
Time: 4.8s
Alternatives: 13
Speedup: 1.8×

Specification

?
\[\begin{array}{l} \\ \begin{array}{l} t_1 := \frac{\cos th}{\sqrt{2}}\\ t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2 \cdot a2\right) \end{array} \end{array} \]
(FPCore (a1 a2 th)
 :precision binary64
 (let* ((t_1 (/ (cos th) (sqrt 2.0))))
   (+ (* t_1 (* a1 a1)) (* t_1 (* a2 a2)))))
double code(double a1, double a2, double th) {
	double t_1 = cos(th) / sqrt(2.0);
	return (t_1 * (a1 * a1)) + (t_1 * (a2 * a2));
}
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(a1, a2, th)
use fmin_fmax_functions
    real(8), intent (in) :: a1
    real(8), intent (in) :: a2
    real(8), intent (in) :: th
    real(8) :: t_1
    t_1 = cos(th) / sqrt(2.0d0)
    code = (t_1 * (a1 * a1)) + (t_1 * (a2 * a2))
end function
public static double code(double a1, double a2, double th) {
	double t_1 = Math.cos(th) / Math.sqrt(2.0);
	return (t_1 * (a1 * a1)) + (t_1 * (a2 * a2));
}
def code(a1, a2, th):
	t_1 = math.cos(th) / math.sqrt(2.0)
	return (t_1 * (a1 * a1)) + (t_1 * (a2 * a2))
function code(a1, a2, th)
	t_1 = Float64(cos(th) / sqrt(2.0))
	return Float64(Float64(t_1 * Float64(a1 * a1)) + Float64(t_1 * Float64(a2 * a2)))
end
function tmp = code(a1, a2, th)
	t_1 = cos(th) / sqrt(2.0);
	tmp = (t_1 * (a1 * a1)) + (t_1 * (a2 * a2));
end
code[a1_, a2_, th_] := Block[{t$95$1 = N[(N[Cos[th], $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]}, N[(N[(t$95$1 * N[(a1 * a1), $MachinePrecision]), $MachinePrecision] + N[(t$95$1 * N[(a2 * a2), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_1 := \frac{\cos th}{\sqrt{2}}\\
t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2 \cdot a2\right)
\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 13 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: 99.5% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_1 := \frac{\cos th}{\sqrt{2}}\\ t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2 \cdot a2\right) \end{array} \end{array} \]
(FPCore (a1 a2 th)
 :precision binary64
 (let* ((t_1 (/ (cos th) (sqrt 2.0))))
   (+ (* t_1 (* a1 a1)) (* t_1 (* a2 a2)))))
double code(double a1, double a2, double th) {
	double t_1 = cos(th) / sqrt(2.0);
	return (t_1 * (a1 * a1)) + (t_1 * (a2 * a2));
}
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(a1, a2, th)
use fmin_fmax_functions
    real(8), intent (in) :: a1
    real(8), intent (in) :: a2
    real(8), intent (in) :: th
    real(8) :: t_1
    t_1 = cos(th) / sqrt(2.0d0)
    code = (t_1 * (a1 * a1)) + (t_1 * (a2 * a2))
end function
public static double code(double a1, double a2, double th) {
	double t_1 = Math.cos(th) / Math.sqrt(2.0);
	return (t_1 * (a1 * a1)) + (t_1 * (a2 * a2));
}
def code(a1, a2, th):
	t_1 = math.cos(th) / math.sqrt(2.0)
	return (t_1 * (a1 * a1)) + (t_1 * (a2 * a2))
function code(a1, a2, th)
	t_1 = Float64(cos(th) / sqrt(2.0))
	return Float64(Float64(t_1 * Float64(a1 * a1)) + Float64(t_1 * Float64(a2 * a2)))
end
function tmp = code(a1, a2, th)
	t_1 = cos(th) / sqrt(2.0);
	tmp = (t_1 * (a1 * a1)) + (t_1 * (a2 * a2));
end
code[a1_, a2_, th_] := Block[{t$95$1 = N[(N[Cos[th], $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]}, N[(N[(t$95$1 * N[(a1 * a1), $MachinePrecision]), $MachinePrecision] + N[(t$95$1 * N[(a2 * a2), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_1 := \frac{\cos th}{\sqrt{2}}\\
t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2 \cdot a2\right)
\end{array}
\end{array}

Alternative 1: 99.6% accurate, 1.0× speedup?

\[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \mathsf{fma}\left(\cos th, a2\_m \cdot \frac{a2\_m}{\sqrt{2}}, \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1\right) \end{array} \]
a2_m = (fabs.f64 a2)
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
(FPCore (a1 a2_m th)
 :precision binary64
 (fma
  (cos th)
  (* a2_m (/ a2_m (sqrt 2.0)))
  (* (/ (* (cos th) a1) (sqrt 2.0)) a1)))
a2_m = fabs(a2);
assert(a1 < a2_m && a2_m < th);
double code(double a1, double a2_m, double th) {
	return fma(cos(th), (a2_m * (a2_m / sqrt(2.0))), (((cos(th) * a1) / sqrt(2.0)) * a1));
}
a2_m = abs(a2)
a1, a2_m, th = sort([a1, a2_m, th])
function code(a1, a2_m, th)
	return fma(cos(th), Float64(a2_m * Float64(a2_m / sqrt(2.0))), Float64(Float64(Float64(cos(th) * a1) / sqrt(2.0)) * a1))
end
a2_m = N[Abs[a2], $MachinePrecision]
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
code[a1_, a2$95$m_, th_] := N[(N[Cos[th], $MachinePrecision] * N[(a2$95$m * N[(a2$95$m / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(N[(N[(N[Cos[th], $MachinePrecision] * a1), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision] * a1), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
a2_m = \left|a2\right|
\\
[a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
\\
\mathsf{fma}\left(\cos th, a2\_m \cdot \frac{a2\_m}{\sqrt{2}}, \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1\right)
\end{array}
Derivation
  1. Initial program 99.5%

    \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
  2. Step-by-step derivation
    1. lift-+.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    2. lift-*.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    3. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    4. lift-cos.f64N/A

      \[\leadsto \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    5. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    6. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    7. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    8. lift-/.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    9. lift-cos.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    10. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    11. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a2 \cdot a2\right)} \]
    12. +-commutativeN/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} \]
    13. pow2N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    14. associate-*l/N/A

      \[\leadsto \color{blue}{\frac{\cos th \cdot {a2}^{2}}{\sqrt{2}}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    15. associate-/l*N/A

      \[\leadsto \color{blue}{\cos th \cdot \frac{{a2}^{2}}{\sqrt{2}}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    16. lower-fma.f64N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left(\cos th, \frac{{a2}^{2}}{\sqrt{2}}, \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)\right)} \]
  3. Applied rewrites99.6%

    \[\leadsto \color{blue}{\mathsf{fma}\left(\cos th, a2 \cdot \frac{a2}{\sqrt{2}}, \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1\right)} \]
  4. Add Preprocessing

Alternative 2: 99.6% accurate, 1.0× speedup?

\[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \mathsf{fma}\left(\frac{\cos th \cdot a2\_m}{\sqrt{2}}, a2\_m, \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1\right) \end{array} \]
a2_m = (fabs.f64 a2)
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
(FPCore (a1 a2_m th)
 :precision binary64
 (fma
  (/ (* (cos th) a2_m) (sqrt 2.0))
  a2_m
  (* (/ (* (cos th) a1) (sqrt 2.0)) a1)))
a2_m = fabs(a2);
assert(a1 < a2_m && a2_m < th);
double code(double a1, double a2_m, double th) {
	return fma(((cos(th) * a2_m) / sqrt(2.0)), a2_m, (((cos(th) * a1) / sqrt(2.0)) * a1));
}
a2_m = abs(a2)
a1, a2_m, th = sort([a1, a2_m, th])
function code(a1, a2_m, th)
	return fma(Float64(Float64(cos(th) * a2_m) / sqrt(2.0)), a2_m, Float64(Float64(Float64(cos(th) * a1) / sqrt(2.0)) * a1))
end
a2_m = N[Abs[a2], $MachinePrecision]
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
code[a1_, a2$95$m_, th_] := N[(N[(N[(N[Cos[th], $MachinePrecision] * a2$95$m), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision] * a2$95$m + N[(N[(N[(N[Cos[th], $MachinePrecision] * a1), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision] * a1), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
a2_m = \left|a2\right|
\\
[a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
\\
\mathsf{fma}\left(\frac{\cos th \cdot a2\_m}{\sqrt{2}}, a2\_m, \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1\right)
\end{array}
Derivation
  1. Initial program 99.5%

    \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
  2. Step-by-step derivation
    1. lift-+.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    2. lift-*.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    3. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    4. lift-cos.f64N/A

      \[\leadsto \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    5. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    6. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    7. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    8. lift-/.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    9. lift-cos.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    10. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    11. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a2 \cdot a2\right)} \]
    12. +-commutativeN/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} \]
    13. associate-*r*N/A

      \[\leadsto \color{blue}{\left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot a2} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    14. lower-fma.f64N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{\cos th}{\sqrt{2}} \cdot a2, a2, \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)\right)} \]
  3. Applied rewrites99.6%

    \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{\cos th \cdot a2}{\sqrt{2}}, a2, \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1\right)} \]
  4. Add Preprocessing

Alternative 3: 99.6% accurate, 1.0× speedup?

\[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \mathsf{fma}\left(\cos th \cdot \frac{a1}{\sqrt{2}}, a1, \left(\cos th \cdot a2\_m\right) \cdot \frac{a2\_m}{\sqrt{2}}\right) \end{array} \]
a2_m = (fabs.f64 a2)
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
(FPCore (a1 a2_m th)
 :precision binary64
 (fma
  (* (cos th) (/ a1 (sqrt 2.0)))
  a1
  (* (* (cos th) a2_m) (/ a2_m (sqrt 2.0)))))
a2_m = fabs(a2);
assert(a1 < a2_m && a2_m < th);
double code(double a1, double a2_m, double th) {
	return fma((cos(th) * (a1 / sqrt(2.0))), a1, ((cos(th) * a2_m) * (a2_m / sqrt(2.0))));
}
a2_m = abs(a2)
a1, a2_m, th = sort([a1, a2_m, th])
function code(a1, a2_m, th)
	return fma(Float64(cos(th) * Float64(a1 / sqrt(2.0))), a1, Float64(Float64(cos(th) * a2_m) * Float64(a2_m / sqrt(2.0))))
end
a2_m = N[Abs[a2], $MachinePrecision]
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
code[a1_, a2$95$m_, th_] := N[(N[(N[Cos[th], $MachinePrecision] * N[(a1 / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * a1 + N[(N[(N[Cos[th], $MachinePrecision] * a2$95$m), $MachinePrecision] * N[(a2$95$m / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
a2_m = \left|a2\right|
\\
[a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
\\
\mathsf{fma}\left(\cos th \cdot \frac{a1}{\sqrt{2}}, a1, \left(\cos th \cdot a2\_m\right) \cdot \frac{a2\_m}{\sqrt{2}}\right)
\end{array}
Derivation
  1. Initial program 99.5%

    \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
  2. Step-by-step derivation
    1. lift-+.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    2. lift-*.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    3. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    4. lift-cos.f64N/A

      \[\leadsto \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    5. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    6. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    7. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    8. lift-/.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    9. lift-cos.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    10. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    11. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a2 \cdot a2\right)} \]
    12. +-commutativeN/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} \]
    13. pow2N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    14. associate-*l/N/A

      \[\leadsto \color{blue}{\frac{\cos th \cdot {a2}^{2}}{\sqrt{2}}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    15. associate-/l*N/A

      \[\leadsto \color{blue}{\cos th \cdot \frac{{a2}^{2}}{\sqrt{2}}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    16. lower-fma.f64N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left(\cos th, \frac{{a2}^{2}}{\sqrt{2}}, \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)\right)} \]
  3. Applied rewrites99.6%

    \[\leadsto \color{blue}{\mathsf{fma}\left(\cos th, a2 \cdot \frac{a2}{\sqrt{2}}, \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1\right)} \]
  4. Step-by-step derivation
    1. lift-cos.f64N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\cos th}, a2 \cdot \frac{a2}{\sqrt{2}}, \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1\right) \]
    2. lift-fma.f64N/A

      \[\leadsto \color{blue}{\cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right) + \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1} \]
    3. lift-*.f64N/A

      \[\leadsto \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right) + \color{blue}{\frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1} \]
    4. lift-/.f64N/A

      \[\leadsto \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right) + \color{blue}{\frac{\cos th \cdot a1}{\sqrt{2}}} \cdot a1 \]
    5. lift-*.f64N/A

      \[\leadsto \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right) + \frac{\color{blue}{\cos th \cdot a1}}{\sqrt{2}} \cdot a1 \]
    6. lift-cos.f64N/A

      \[\leadsto \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right) + \frac{\color{blue}{\cos th} \cdot a1}{\sqrt{2}} \cdot a1 \]
    7. lift-sqrt.f64N/A

      \[\leadsto \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right) + \frac{\cos th \cdot a1}{\color{blue}{\sqrt{2}}} \cdot a1 \]
    8. +-commutativeN/A

      \[\leadsto \color{blue}{\frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1 + \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right)} \]
    9. lower-fma.f64N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{\cos th \cdot a1}{\sqrt{2}}, a1, \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right)\right)} \]
    10. associate-/l*N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\cos th \cdot \frac{a1}{\sqrt{2}}}, a1, \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right)\right) \]
    11. lower-*.f64N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\cos th \cdot \frac{a1}{\sqrt{2}}}, a1, \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right)\right) \]
    12. lift-cos.f64N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\cos th} \cdot \frac{a1}{\sqrt{2}}, a1, \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right)\right) \]
    13. lower-/.f64N/A

      \[\leadsto \mathsf{fma}\left(\cos th \cdot \color{blue}{\frac{a1}{\sqrt{2}}}, a1, \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right)\right) \]
    14. lift-sqrt.f64N/A

      \[\leadsto \mathsf{fma}\left(\cos th \cdot \frac{a1}{\color{blue}{\sqrt{2}}}, a1, \cos th \cdot \left(a2 \cdot \frac{a2}{\sqrt{2}}\right)\right) \]
    15. lift-*.f64N/A

      \[\leadsto \mathsf{fma}\left(\cos th \cdot \frac{a1}{\sqrt{2}}, a1, \cos th \cdot \color{blue}{\left(a2 \cdot \frac{a2}{\sqrt{2}}\right)}\right) \]
    16. lift-/.f64N/A

      \[\leadsto \mathsf{fma}\left(\cos th \cdot \frac{a1}{\sqrt{2}}, a1, \cos th \cdot \left(a2 \cdot \color{blue}{\frac{a2}{\sqrt{2}}}\right)\right) \]
    17. lift-sqrt.f64N/A

      \[\leadsto \mathsf{fma}\left(\cos th \cdot \frac{a1}{\sqrt{2}}, a1, \cos th \cdot \left(a2 \cdot \frac{a2}{\color{blue}{\sqrt{2}}}\right)\right) \]
  5. Applied rewrites99.6%

    \[\leadsto \color{blue}{\mathsf{fma}\left(\cos th \cdot \frac{a1}{\sqrt{2}}, a1, \left(\cos th \cdot a2\right) \cdot \frac{a2}{\sqrt{2}}\right)} \]
  6. Add Preprocessing

Alternative 4: 99.6% accurate, 1.8× speedup?

\[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \frac{\cos th \cdot \mathsf{fma}\left(a1, a1, a2\_m \cdot a2\_m\right)}{\sqrt{2}} \end{array} \]
a2_m = (fabs.f64 a2)
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
(FPCore (a1 a2_m th)
 :precision binary64
 (/ (* (cos th) (fma a1 a1 (* a2_m a2_m))) (sqrt 2.0)))
a2_m = fabs(a2);
assert(a1 < a2_m && a2_m < th);
double code(double a1, double a2_m, double th) {
	return (cos(th) * fma(a1, a1, (a2_m * a2_m))) / sqrt(2.0);
}
a2_m = abs(a2)
a1, a2_m, th = sort([a1, a2_m, th])
function code(a1, a2_m, th)
	return Float64(Float64(cos(th) * fma(a1, a1, Float64(a2_m * a2_m))) / sqrt(2.0))
end
a2_m = N[Abs[a2], $MachinePrecision]
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
code[a1_, a2$95$m_, th_] := N[(N[(N[Cos[th], $MachinePrecision] * N[(a1 * a1 + N[(a2$95$m * a2$95$m), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
a2_m = \left|a2\right|
\\
[a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
\\
\frac{\cos th \cdot \mathsf{fma}\left(a1, a1, a2\_m \cdot a2\_m\right)}{\sqrt{2}}
\end{array}
Derivation
  1. Initial program 99.5%

    \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
  2. Step-by-step derivation
    1. lift-+.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    2. lift-*.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    3. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    4. lift-cos.f64N/A

      \[\leadsto \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    5. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    6. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    7. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    8. lift-/.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    9. lift-cos.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    10. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    11. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a2 \cdot a2\right)} \]
    12. pow2N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a1}^{2}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    13. pow2N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot {a1}^{2} + \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} \]
    14. distribute-lft-outN/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left({a1}^{2} + {a2}^{2}\right)} \]
    15. associate-*l/N/A

      \[\leadsto \color{blue}{\frac{\cos th \cdot \left({a1}^{2} + {a2}^{2}\right)}{\sqrt{2}}} \]
    16. distribute-rgt-outN/A

      \[\leadsto \frac{\color{blue}{{a1}^{2} \cdot \cos th + {a2}^{2} \cdot \cos th}}{\sqrt{2}} \]
  3. Applied rewrites99.6%

    \[\leadsto \color{blue}{\frac{\cos th \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}{\sqrt{2}}} \]
  4. Add Preprocessing

Alternative 5: 99.6% accurate, 1.8× speedup?

\[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \cos th \cdot \frac{\mathsf{fma}\left(a1, a1, a2\_m \cdot a2\_m\right)}{\sqrt{2}} \end{array} \]
a2_m = (fabs.f64 a2)
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
(FPCore (a1 a2_m th)
 :precision binary64
 (* (cos th) (/ (fma a1 a1 (* a2_m a2_m)) (sqrt 2.0))))
a2_m = fabs(a2);
assert(a1 < a2_m && a2_m < th);
double code(double a1, double a2_m, double th) {
	return cos(th) * (fma(a1, a1, (a2_m * a2_m)) / sqrt(2.0));
}
a2_m = abs(a2)
a1, a2_m, th = sort([a1, a2_m, th])
function code(a1, a2_m, th)
	return Float64(cos(th) * Float64(fma(a1, a1, Float64(a2_m * a2_m)) / sqrt(2.0)))
end
a2_m = N[Abs[a2], $MachinePrecision]
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
code[a1_, a2$95$m_, th_] := N[(N[Cos[th], $MachinePrecision] * N[(N[(a1 * a1 + N[(a2$95$m * a2$95$m), $MachinePrecision]), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
a2_m = \left|a2\right|
\\
[a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
\\
\cos th \cdot \frac{\mathsf{fma}\left(a1, a1, a2\_m \cdot a2\_m\right)}{\sqrt{2}}
\end{array}
Derivation
  1. Initial program 99.5%

    \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
  2. Step-by-step derivation
    1. lift-+.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    2. lift-*.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    3. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    4. lift-cos.f64N/A

      \[\leadsto \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    5. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    6. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    7. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    8. lift-/.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    9. lift-cos.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    10. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    11. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a2 \cdot a2\right)} \]
    12. pow2N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a1}^{2}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    13. pow2N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot {a1}^{2} + \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} \]
    14. distribute-lft-outN/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left({a1}^{2} + {a2}^{2}\right)} \]
    15. associate-*l/N/A

      \[\leadsto \color{blue}{\frac{\cos th \cdot \left({a1}^{2} + {a2}^{2}\right)}{\sqrt{2}}} \]
    16. distribute-rgt-outN/A

      \[\leadsto \frac{\color{blue}{{a1}^{2} \cdot \cos th + {a2}^{2} \cdot \cos th}}{\sqrt{2}} \]
  3. Applied rewrites99.6%

    \[\leadsto \color{blue}{\frac{\cos th \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}{\sqrt{2}}} \]
  4. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}{\sqrt{2}}} \]
    2. lift-*.f64N/A

      \[\leadsto \frac{\color{blue}{\cos th \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}}{\sqrt{2}} \]
    3. lift-cos.f64N/A

      \[\leadsto \frac{\color{blue}{\cos th} \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}{\sqrt{2}} \]
    4. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}{\color{blue}{\sqrt{2}}} \]
    5. associate-/l*N/A

      \[\leadsto \color{blue}{\cos th \cdot \frac{\mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}{\sqrt{2}}} \]
    6. lift-*.f64N/A

      \[\leadsto \cos th \cdot \frac{\mathsf{fma}\left(a1, a1, \color{blue}{a2 \cdot a2}\right)}{\sqrt{2}} \]
    7. lift-fma.f64N/A

      \[\leadsto \cos th \cdot \frac{\color{blue}{a1 \cdot a1 + a2 \cdot a2}}{\sqrt{2}} \]
    8. pow2N/A

      \[\leadsto \cos th \cdot \frac{\color{blue}{{a1}^{2}} + a2 \cdot a2}{\sqrt{2}} \]
    9. pow2N/A

      \[\leadsto \cos th \cdot \frac{{a1}^{2} + \color{blue}{{a2}^{2}}}{\sqrt{2}} \]
    10. div-add-revN/A

      \[\leadsto \cos th \cdot \color{blue}{\left(\frac{{a1}^{2}}{\sqrt{2}} + \frac{{a2}^{2}}{\sqrt{2}}\right)} \]
    11. lower-*.f64N/A

      \[\leadsto \color{blue}{\cos th \cdot \left(\frac{{a1}^{2}}{\sqrt{2}} + \frac{{a2}^{2}}{\sqrt{2}}\right)} \]
    12. lift-cos.f64N/A

      \[\leadsto \color{blue}{\cos th} \cdot \left(\frac{{a1}^{2}}{\sqrt{2}} + \frac{{a2}^{2}}{\sqrt{2}}\right) \]
    13. div-add-revN/A

      \[\leadsto \cos th \cdot \color{blue}{\frac{{a1}^{2} + {a2}^{2}}{\sqrt{2}}} \]
    14. lower-/.f64N/A

      \[\leadsto \cos th \cdot \color{blue}{\frac{{a1}^{2} + {a2}^{2}}{\sqrt{2}}} \]
    15. pow2N/A

      \[\leadsto \cos th \cdot \frac{\color{blue}{a1 \cdot a1} + {a2}^{2}}{\sqrt{2}} \]
    16. pow2N/A

      \[\leadsto \cos th \cdot \frac{a1 \cdot a1 + \color{blue}{a2 \cdot a2}}{\sqrt{2}} \]
    17. lift-fma.f64N/A

      \[\leadsto \cos th \cdot \frac{\color{blue}{\mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}}{\sqrt{2}} \]
    18. lift-*.f64N/A

      \[\leadsto \cos th \cdot \frac{\mathsf{fma}\left(a1, a1, \color{blue}{a2 \cdot a2}\right)}{\sqrt{2}} \]
    19. lift-sqrt.f6499.6

      \[\leadsto \cos th \cdot \frac{\mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}{\color{blue}{\sqrt{2}}} \]
  5. Applied rewrites99.6%

    \[\leadsto \color{blue}{\cos th \cdot \frac{\mathsf{fma}\left(a1, a1, a2 \cdot a2\right)}{\sqrt{2}}} \]
  6. Add Preprocessing

Alternative 6: 78.1% accurate, 2.0× speedup?

\[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \left(\cos th \cdot \frac{a2\_m}{\sqrt{2}}\right) \cdot a2\_m \end{array} \]
a2_m = (fabs.f64 a2)
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
(FPCore (a1 a2_m th)
 :precision binary64
 (* (* (cos th) (/ a2_m (sqrt 2.0))) a2_m))
a2_m = fabs(a2);
assert(a1 < a2_m && a2_m < th);
double code(double a1, double a2_m, double th) {
	return (cos(th) * (a2_m / sqrt(2.0))) * a2_m;
}
a2_m =     private
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
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(a1, a2_m, th)
use fmin_fmax_functions
    real(8), intent (in) :: a1
    real(8), intent (in) :: a2_m
    real(8), intent (in) :: th
    code = (cos(th) * (a2_m / sqrt(2.0d0))) * a2_m
end function
a2_m = Math.abs(a2);
assert a1 < a2_m && a2_m < th;
public static double code(double a1, double a2_m, double th) {
	return (Math.cos(th) * (a2_m / Math.sqrt(2.0))) * a2_m;
}
a2_m = math.fabs(a2)
[a1, a2_m, th] = sort([a1, a2_m, th])
def code(a1, a2_m, th):
	return (math.cos(th) * (a2_m / math.sqrt(2.0))) * a2_m
a2_m = abs(a2)
a1, a2_m, th = sort([a1, a2_m, th])
function code(a1, a2_m, th)
	return Float64(Float64(cos(th) * Float64(a2_m / sqrt(2.0))) * a2_m)
end
a2_m = abs(a2);
a1, a2_m, th = num2cell(sort([a1, a2_m, th])){:}
function tmp = code(a1, a2_m, th)
	tmp = (cos(th) * (a2_m / sqrt(2.0))) * a2_m;
end
a2_m = N[Abs[a2], $MachinePrecision]
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
code[a1_, a2$95$m_, th_] := N[(N[(N[Cos[th], $MachinePrecision] * N[(a2$95$m / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * a2$95$m), $MachinePrecision]
\begin{array}{l}
a2_m = \left|a2\right|
\\
[a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
\\
\left(\cos th \cdot \frac{a2\_m}{\sqrt{2}}\right) \cdot a2\_m
\end{array}
Derivation
  1. Initial program 99.5%

    \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
  2. Taylor expanded in a1 around 0

    \[\leadsto \color{blue}{\frac{{a2}^{2} \cdot \cos th}{\sqrt{2}}} \]
  3. Step-by-step derivation
    1. associate-/l*N/A

      \[\leadsto {a2}^{2} \cdot \color{blue}{\frac{\cos th}{\sqrt{2}}} \]
    2. *-commutativeN/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} \]
    3. pow2N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot \color{blue}{a2}\right) \]
    4. associate-*r*N/A

      \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot \color{blue}{a2} \]
    5. lower-*.f64N/A

      \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot \color{blue}{a2} \]
    6. associate-*l/N/A

      \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
    7. lower-/.f64N/A

      \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
    8. lower-*.f64N/A

      \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
    9. lift-cos.f64N/A

      \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
    10. lift-sqrt.f6478.1

      \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
  4. Applied rewrites78.1%

    \[\leadsto \color{blue}{\frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2} \]
  5. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
    2. lift-*.f64N/A

      \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
    3. lift-cos.f64N/A

      \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
    4. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
    5. associate-/l*N/A

      \[\leadsto \left(\cos th \cdot \frac{a2}{\sqrt{2}}\right) \cdot a2 \]
    6. lower-*.f64N/A

      \[\leadsto \left(\cos th \cdot \frac{a2}{\sqrt{2}}\right) \cdot a2 \]
    7. lift-cos.f64N/A

      \[\leadsto \left(\cos th \cdot \frac{a2}{\sqrt{2}}\right) \cdot a2 \]
    8. lift-sqrt.f64N/A

      \[\leadsto \left(\cos th \cdot \frac{a2}{\sqrt{2}}\right) \cdot a2 \]
    9. lift-/.f6478.1

      \[\leadsto \left(\cos th \cdot \frac{a2}{\sqrt{2}}\right) \cdot a2 \]
  6. Applied rewrites78.1%

    \[\leadsto \left(\cos th \cdot \frac{a2}{\sqrt{2}}\right) \cdot \color{blue}{a2} \]
  7. Add Preprocessing

Alternative 7: 78.1% accurate, 2.0× speedup?

\[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \left(\frac{\cos th}{\sqrt{2}} \cdot a2\_m\right) \cdot a2\_m \end{array} \]
a2_m = (fabs.f64 a2)
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
(FPCore (a1 a2_m th)
 :precision binary64
 (* (* (/ (cos th) (sqrt 2.0)) a2_m) a2_m))
a2_m = fabs(a2);
assert(a1 < a2_m && a2_m < th);
double code(double a1, double a2_m, double th) {
	return ((cos(th) / sqrt(2.0)) * a2_m) * a2_m;
}
a2_m =     private
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
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(a1, a2_m, th)
use fmin_fmax_functions
    real(8), intent (in) :: a1
    real(8), intent (in) :: a2_m
    real(8), intent (in) :: th
    code = ((cos(th) / sqrt(2.0d0)) * a2_m) * a2_m
end function
a2_m = Math.abs(a2);
assert a1 < a2_m && a2_m < th;
public static double code(double a1, double a2_m, double th) {
	return ((Math.cos(th) / Math.sqrt(2.0)) * a2_m) * a2_m;
}
a2_m = math.fabs(a2)
[a1, a2_m, th] = sort([a1, a2_m, th])
def code(a1, a2_m, th):
	return ((math.cos(th) / math.sqrt(2.0)) * a2_m) * a2_m
a2_m = abs(a2)
a1, a2_m, th = sort([a1, a2_m, th])
function code(a1, a2_m, th)
	return Float64(Float64(Float64(cos(th) / sqrt(2.0)) * a2_m) * a2_m)
end
a2_m = abs(a2);
a1, a2_m, th = num2cell(sort([a1, a2_m, th])){:}
function tmp = code(a1, a2_m, th)
	tmp = ((cos(th) / sqrt(2.0)) * a2_m) * a2_m;
end
a2_m = N[Abs[a2], $MachinePrecision]
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
code[a1_, a2$95$m_, th_] := N[(N[(N[(N[Cos[th], $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision] * a2$95$m), $MachinePrecision] * a2$95$m), $MachinePrecision]
\begin{array}{l}
a2_m = \left|a2\right|
\\
[a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
\\
\left(\frac{\cos th}{\sqrt{2}} \cdot a2\_m\right) \cdot a2\_m
\end{array}
Derivation
  1. Initial program 99.5%

    \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
  2. Step-by-step derivation
    1. lift-+.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    2. lift-*.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    3. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    4. lift-cos.f64N/A

      \[\leadsto \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    5. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    6. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    7. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
    8. lift-/.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    9. lift-cos.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    10. lift-sqrt.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
    11. lift-*.f64N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a2 \cdot a2\right)} \]
    12. +-commutativeN/A

      \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} \]
    13. pow2N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    14. associate-*l/N/A

      \[\leadsto \color{blue}{\frac{\cos th \cdot {a2}^{2}}{\sqrt{2}}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    15. associate-/l*N/A

      \[\leadsto \color{blue}{\cos th \cdot \frac{{a2}^{2}}{\sqrt{2}}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) \]
    16. lower-fma.f64N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left(\cos th, \frac{{a2}^{2}}{\sqrt{2}}, \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)\right)} \]
  3. Applied rewrites99.6%

    \[\leadsto \color{blue}{\mathsf{fma}\left(\cos th, a2 \cdot \frac{a2}{\sqrt{2}}, \frac{\cos th \cdot a1}{\sqrt{2}} \cdot a1\right)} \]
  4. Taylor expanded in a1 around 0

    \[\leadsto \color{blue}{\frac{{a2}^{2} \cdot \cos th}{\sqrt{2}}} \]
  5. Step-by-step derivation
    1. associate-/l*N/A

      \[\leadsto {a2}^{2} \cdot \color{blue}{\frac{\cos th}{\sqrt{2}}} \]
    2. *-commutativeN/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} \]
    3. pow2N/A

      \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot \color{blue}{a2}\right) \]
    4. associate-*r*N/A

      \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot \color{blue}{a2} \]
    5. lower-*.f64N/A

      \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot \color{blue}{a2} \]
    6. lower-*.f64N/A

      \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot a2 \]
    7. lift-cos.f64N/A

      \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot a2 \]
    8. lift-sqrt.f64N/A

      \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot a2 \]
    9. lift-/.f6478.1

      \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot a2 \]
  6. Applied rewrites78.1%

    \[\leadsto \color{blue}{\left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot a2} \]
  7. Add Preprocessing

Alternative 8: 76.8% accurate, 0.8× speedup?

\[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \begin{array}{l} t_1 := \frac{\cos th}{\sqrt{2}}\\ \mathbf{if}\;t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2\_m \cdot a2\_m\right) \leq -1 \cdot 10^{-94}:\\ \;\;\;\;\frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2\_m, -0.5, a2\_m\right)}{\sqrt{2}} \cdot a2\_m\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(1, a1 \cdot \frac{a1}{\sqrt{2}}, \frac{1 \cdot a2\_m}{\sqrt{2}} \cdot a2\_m\right)\\ \end{array} \end{array} \]
a2_m = (fabs.f64 a2)
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
(FPCore (a1 a2_m th)
 :precision binary64
 (let* ((t_1 (/ (cos th) (sqrt 2.0))))
   (if (<= (+ (* t_1 (* a1 a1)) (* t_1 (* a2_m a2_m))) -1e-94)
     (* (/ (fma (* (* th th) a2_m) -0.5 a2_m) (sqrt 2.0)) a2_m)
     (fma 1.0 (* a1 (/ a1 (sqrt 2.0))) (* (/ (* 1.0 a2_m) (sqrt 2.0)) a2_m)))))
a2_m = fabs(a2);
assert(a1 < a2_m && a2_m < th);
double code(double a1, double a2_m, double th) {
	double t_1 = cos(th) / sqrt(2.0);
	double tmp;
	if (((t_1 * (a1 * a1)) + (t_1 * (a2_m * a2_m))) <= -1e-94) {
		tmp = (fma(((th * th) * a2_m), -0.5, a2_m) / sqrt(2.0)) * a2_m;
	} else {
		tmp = fma(1.0, (a1 * (a1 / sqrt(2.0))), (((1.0 * a2_m) / sqrt(2.0)) * a2_m));
	}
	return tmp;
}
a2_m = abs(a2)
a1, a2_m, th = sort([a1, a2_m, th])
function code(a1, a2_m, th)
	t_1 = Float64(cos(th) / sqrt(2.0))
	tmp = 0.0
	if (Float64(Float64(t_1 * Float64(a1 * a1)) + Float64(t_1 * Float64(a2_m * a2_m))) <= -1e-94)
		tmp = Float64(Float64(fma(Float64(Float64(th * th) * a2_m), -0.5, a2_m) / sqrt(2.0)) * a2_m);
	else
		tmp = fma(1.0, Float64(a1 * Float64(a1 / sqrt(2.0))), Float64(Float64(Float64(1.0 * a2_m) / sqrt(2.0)) * a2_m));
	end
	return tmp
end
a2_m = N[Abs[a2], $MachinePrecision]
NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
code[a1_, a2$95$m_, th_] := Block[{t$95$1 = N[(N[Cos[th], $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[N[(N[(t$95$1 * N[(a1 * a1), $MachinePrecision]), $MachinePrecision] + N[(t$95$1 * N[(a2$95$m * a2$95$m), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], -1e-94], N[(N[(N[(N[(N[(th * th), $MachinePrecision] * a2$95$m), $MachinePrecision] * -0.5 + a2$95$m), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision] * a2$95$m), $MachinePrecision], N[(1.0 * N[(a1 * N[(a1 / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(N[(N[(1.0 * a2$95$m), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision] * a2$95$m), $MachinePrecision]), $MachinePrecision]]]
\begin{array}{l}
a2_m = \left|a2\right|
\\
[a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
\\
\begin{array}{l}
t_1 := \frac{\cos th}{\sqrt{2}}\\
\mathbf{if}\;t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2\_m \cdot a2\_m\right) \leq -1 \cdot 10^{-94}:\\
\;\;\;\;\frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2\_m, -0.5, a2\_m\right)}{\sqrt{2}} \cdot a2\_m\\

\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(1, a1 \cdot \frac{a1}{\sqrt{2}}, \frac{1 \cdot a2\_m}{\sqrt{2}} \cdot a2\_m\right)\\


\end{array}
\end{array}
Derivation
  1. Split input into 2 regimes
  2. if (+.f64 (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a1 a1)) (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a2 a2))) < -9.9999999999999996e-95

    1. Initial program 99.5%

      \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    2. Taylor expanded in a1 around 0

      \[\leadsto \color{blue}{\frac{{a2}^{2} \cdot \cos th}{\sqrt{2}}} \]
    3. Step-by-step derivation
      1. associate-/l*N/A

        \[\leadsto {a2}^{2} \cdot \color{blue}{\frac{\cos th}{\sqrt{2}}} \]
      2. *-commutativeN/A

        \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} \]
      3. pow2N/A

        \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot \color{blue}{a2}\right) \]
      4. associate-*r*N/A

        \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot \color{blue}{a2} \]
      5. lower-*.f64N/A

        \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot \color{blue}{a2} \]
      6. associate-*l/N/A

        \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
      7. lower-/.f64N/A

        \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
      8. lower-*.f64N/A

        \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
      9. lift-cos.f64N/A

        \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
      10. lift-sqrt.f6478.1

        \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
    4. Applied rewrites78.1%

      \[\leadsto \color{blue}{\frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2} \]
    5. Taylor expanded in th around 0

      \[\leadsto \frac{a2 + \frac{-1}{2} \cdot \left(a2 \cdot {th}^{2}\right)}{\sqrt{2}} \cdot a2 \]
    6. Step-by-step derivation
      1. +-commutativeN/A

        \[\leadsto \frac{\frac{-1}{2} \cdot \left(a2 \cdot {th}^{2}\right) + a2}{\sqrt{2}} \cdot a2 \]
      2. *-commutativeN/A

        \[\leadsto \frac{\left(a2 \cdot {th}^{2}\right) \cdot \frac{-1}{2} + a2}{\sqrt{2}} \cdot a2 \]
      3. lower-fma.f64N/A

        \[\leadsto \frac{\mathsf{fma}\left(a2 \cdot {th}^{2}, \frac{-1}{2}, a2\right)}{\sqrt{2}} \cdot a2 \]
      4. *-commutativeN/A

        \[\leadsto \frac{\mathsf{fma}\left({th}^{2} \cdot a2, \frac{-1}{2}, a2\right)}{\sqrt{2}} \cdot a2 \]
      5. lower-*.f64N/A

        \[\leadsto \frac{\mathsf{fma}\left({th}^{2} \cdot a2, \frac{-1}{2}, a2\right)}{\sqrt{2}} \cdot a2 \]
      6. pow2N/A

        \[\leadsto \frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2, \frac{-1}{2}, a2\right)}{\sqrt{2}} \cdot a2 \]
      7. lift-*.f6450.8

        \[\leadsto \frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2, -0.5, a2\right)}{\sqrt{2}} \cdot a2 \]
    7. Applied rewrites50.8%

      \[\leadsto \frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2, -0.5, a2\right)}{\sqrt{2}} \cdot a2 \]

    if -9.9999999999999996e-95 < (+.f64 (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a1 a1)) (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a2 a2)))

    1. Initial program 99.5%

      \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
    2. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
      2. lift-*.f64N/A

        \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      3. lift-/.f64N/A

        \[\leadsto \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      4. lift-cos.f64N/A

        \[\leadsto \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      5. lift-sqrt.f64N/A

        \[\leadsto \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      6. lift-*.f64N/A

        \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a1 \cdot a1\right)} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      7. lift-*.f64N/A

        \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
      8. lift-/.f64N/A

        \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\cos th}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
      9. lift-cos.f64N/A

        \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\color{blue}{\cos th}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      10. lift-sqrt.f64N/A

        \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\color{blue}{\sqrt{2}}} \cdot \left(a2 \cdot a2\right) \]
      11. lift-*.f64N/A

        \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{\left(a2 \cdot a2\right)} \]
      12. pow2N/A

        \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a1}^{2}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      13. associate-*l/N/A

        \[\leadsto \color{blue}{\frac{\cos th \cdot {a1}^{2}}{\sqrt{2}}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      14. associate-/l*N/A

        \[\leadsto \color{blue}{\cos th \cdot \frac{{a1}^{2}}{\sqrt{2}}} + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      15. lower-fma.f64N/A

        \[\leadsto \color{blue}{\mathsf{fma}\left(\cos th, \frac{{a1}^{2}}{\sqrt{2}}, \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)\right)} \]
    3. Applied rewrites99.6%

      \[\leadsto \color{blue}{\mathsf{fma}\left(\cos th, a1 \cdot \frac{a1}{\sqrt{2}}, \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2\right)} \]
    4. Taylor expanded in th around 0

      \[\leadsto \mathsf{fma}\left(\color{blue}{1}, a1 \cdot \frac{a1}{\sqrt{2}}, \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2\right) \]
    5. Step-by-step derivation
      1. Applied rewrites90.0%

        \[\leadsto \mathsf{fma}\left(\color{blue}{1}, a1 \cdot \frac{a1}{\sqrt{2}}, \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2\right) \]
      2. Taylor expanded in th around 0

        \[\leadsto \mathsf{fma}\left(1, a1 \cdot \frac{a1}{\sqrt{2}}, \frac{\color{blue}{1} \cdot a2}{\sqrt{2}} \cdot a2\right) \]
      3. Step-by-step derivation
        1. Applied rewrites66.5%

          \[\leadsto \mathsf{fma}\left(1, a1 \cdot \frac{a1}{\sqrt{2}}, \frac{\color{blue}{1} \cdot a2}{\sqrt{2}} \cdot a2\right) \]
      4. Recombined 2 regimes into one program.
      5. Add Preprocessing

      Alternative 9: 76.8% accurate, 0.8× speedup?

      \[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \begin{array}{l} t_1 := \frac{\cos th}{\sqrt{2}}\\ \mathbf{if}\;t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2\_m \cdot a2\_m\right) \leq -1 \cdot 10^{-94}:\\ \;\;\;\;\frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2\_m, -0.5, a2\_m\right)}{\sqrt{2}} \cdot a2\_m\\ \mathbf{else}:\\ \;\;\;\;\frac{\mathsf{fma}\left(a2\_m, a2\_m, a1 \cdot a1\right)}{\sqrt{2}}\\ \end{array} \end{array} \]
      a2_m = (fabs.f64 a2)
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      (FPCore (a1 a2_m th)
       :precision binary64
       (let* ((t_1 (/ (cos th) (sqrt 2.0))))
         (if (<= (+ (* t_1 (* a1 a1)) (* t_1 (* a2_m a2_m))) -1e-94)
           (* (/ (fma (* (* th th) a2_m) -0.5 a2_m) (sqrt 2.0)) a2_m)
           (/ (fma a2_m a2_m (* a1 a1)) (sqrt 2.0)))))
      a2_m = fabs(a2);
      assert(a1 < a2_m && a2_m < th);
      double code(double a1, double a2_m, double th) {
      	double t_1 = cos(th) / sqrt(2.0);
      	double tmp;
      	if (((t_1 * (a1 * a1)) + (t_1 * (a2_m * a2_m))) <= -1e-94) {
      		tmp = (fma(((th * th) * a2_m), -0.5, a2_m) / sqrt(2.0)) * a2_m;
      	} else {
      		tmp = fma(a2_m, a2_m, (a1 * a1)) / sqrt(2.0);
      	}
      	return tmp;
      }
      
      a2_m = abs(a2)
      a1, a2_m, th = sort([a1, a2_m, th])
      function code(a1, a2_m, th)
      	t_1 = Float64(cos(th) / sqrt(2.0))
      	tmp = 0.0
      	if (Float64(Float64(t_1 * Float64(a1 * a1)) + Float64(t_1 * Float64(a2_m * a2_m))) <= -1e-94)
      		tmp = Float64(Float64(fma(Float64(Float64(th * th) * a2_m), -0.5, a2_m) / sqrt(2.0)) * a2_m);
      	else
      		tmp = Float64(fma(a2_m, a2_m, Float64(a1 * a1)) / sqrt(2.0));
      	end
      	return tmp
      end
      
      a2_m = N[Abs[a2], $MachinePrecision]
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      code[a1_, a2$95$m_, th_] := Block[{t$95$1 = N[(N[Cos[th], $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[N[(N[(t$95$1 * N[(a1 * a1), $MachinePrecision]), $MachinePrecision] + N[(t$95$1 * N[(a2$95$m * a2$95$m), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], -1e-94], N[(N[(N[(N[(N[(th * th), $MachinePrecision] * a2$95$m), $MachinePrecision] * -0.5 + a2$95$m), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision] * a2$95$m), $MachinePrecision], N[(N[(a2$95$m * a2$95$m + N[(a1 * a1), $MachinePrecision]), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]]]
      
      \begin{array}{l}
      a2_m = \left|a2\right|
      \\
      [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
      \\
      \begin{array}{l}
      t_1 := \frac{\cos th}{\sqrt{2}}\\
      \mathbf{if}\;t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2\_m \cdot a2\_m\right) \leq -1 \cdot 10^{-94}:\\
      \;\;\;\;\frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2\_m, -0.5, a2\_m\right)}{\sqrt{2}} \cdot a2\_m\\
      
      \mathbf{else}:\\
      \;\;\;\;\frac{\mathsf{fma}\left(a2\_m, a2\_m, a1 \cdot a1\right)}{\sqrt{2}}\\
      
      
      \end{array}
      \end{array}
      
      Derivation
      1. Split input into 2 regimes
      2. if (+.f64 (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a1 a1)) (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a2 a2))) < -9.9999999999999996e-95

        1. Initial program 99.5%

          \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        2. Taylor expanded in a1 around 0

          \[\leadsto \color{blue}{\frac{{a2}^{2} \cdot \cos th}{\sqrt{2}}} \]
        3. Step-by-step derivation
          1. associate-/l*N/A

            \[\leadsto {a2}^{2} \cdot \color{blue}{\frac{\cos th}{\sqrt{2}}} \]
          2. *-commutativeN/A

            \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} \]
          3. pow2N/A

            \[\leadsto \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot \color{blue}{a2}\right) \]
          4. associate-*r*N/A

            \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot \color{blue}{a2} \]
          5. lower-*.f64N/A

            \[\leadsto \left(\frac{\cos th}{\sqrt{2}} \cdot a2\right) \cdot \color{blue}{a2} \]
          6. associate-*l/N/A

            \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
          7. lower-/.f64N/A

            \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
          8. lower-*.f64N/A

            \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
          9. lift-cos.f64N/A

            \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
          10. lift-sqrt.f6478.1

            \[\leadsto \frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2 \]
        4. Applied rewrites78.1%

          \[\leadsto \color{blue}{\frac{\cos th \cdot a2}{\sqrt{2}} \cdot a2} \]
        5. Taylor expanded in th around 0

          \[\leadsto \frac{a2 + \frac{-1}{2} \cdot \left(a2 \cdot {th}^{2}\right)}{\sqrt{2}} \cdot a2 \]
        6. Step-by-step derivation
          1. +-commutativeN/A

            \[\leadsto \frac{\frac{-1}{2} \cdot \left(a2 \cdot {th}^{2}\right) + a2}{\sqrt{2}} \cdot a2 \]
          2. *-commutativeN/A

            \[\leadsto \frac{\left(a2 \cdot {th}^{2}\right) \cdot \frac{-1}{2} + a2}{\sqrt{2}} \cdot a2 \]
          3. lower-fma.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(a2 \cdot {th}^{2}, \frac{-1}{2}, a2\right)}{\sqrt{2}} \cdot a2 \]
          4. *-commutativeN/A

            \[\leadsto \frac{\mathsf{fma}\left({th}^{2} \cdot a2, \frac{-1}{2}, a2\right)}{\sqrt{2}} \cdot a2 \]
          5. lower-*.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left({th}^{2} \cdot a2, \frac{-1}{2}, a2\right)}{\sqrt{2}} \cdot a2 \]
          6. pow2N/A

            \[\leadsto \frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2, \frac{-1}{2}, a2\right)}{\sqrt{2}} \cdot a2 \]
          7. lift-*.f6450.8

            \[\leadsto \frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2, -0.5, a2\right)}{\sqrt{2}} \cdot a2 \]
        7. Applied rewrites50.8%

          \[\leadsto \frac{\mathsf{fma}\left(\left(th \cdot th\right) \cdot a2, -0.5, a2\right)}{\sqrt{2}} \cdot a2 \]

        if -9.9999999999999996e-95 < (+.f64 (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a1 a1)) (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a2 a2)))

        1. Initial program 99.5%

          \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        2. Taylor expanded in th around 0

          \[\leadsto \color{blue}{\frac{{a1}^{2}}{\sqrt{2}} + \frac{{a2}^{2}}{\sqrt{2}}} \]
        3. Step-by-step derivation
          1. +-commutativeN/A

            \[\leadsto \frac{{a2}^{2}}{\sqrt{2}} + \color{blue}{\frac{{a1}^{2}}{\sqrt{2}}} \]
          2. div-add-revN/A

            \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
          3. lower-/.f64N/A

            \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
          4. pow2N/A

            \[\leadsto \frac{a2 \cdot a2 + {a1}^{2}}{\sqrt{2}} \]
          5. lower-fma.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(a2, a2, {a1}^{2}\right)}{\sqrt{\color{blue}{2}}} \]
          6. pow2N/A

            \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
          7. lift-*.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
          8. lift-sqrt.f6466.5

            \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
        4. Applied rewrites66.5%

          \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}}} \]
      3. Recombined 2 regimes into one program.
      4. Add Preprocessing

      Alternative 10: 76.3% accurate, 0.8× speedup?

      \[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \begin{array}{l} t_1 := \frac{\cos th}{\sqrt{2}}\\ \mathbf{if}\;t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2\_m \cdot a2\_m\right) \leq -1 \cdot 10^{-94}:\\ \;\;\;\;\frac{\left(th \cdot th\right) \cdot -0.5}{\sqrt{2}} \cdot \left(a2\_m \cdot a2\_m\right)\\ \mathbf{else}:\\ \;\;\;\;\frac{\mathsf{fma}\left(a2\_m, a2\_m, a1 \cdot a1\right)}{\sqrt{2}}\\ \end{array} \end{array} \]
      a2_m = (fabs.f64 a2)
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      (FPCore (a1 a2_m th)
       :precision binary64
       (let* ((t_1 (/ (cos th) (sqrt 2.0))))
         (if (<= (+ (* t_1 (* a1 a1)) (* t_1 (* a2_m a2_m))) -1e-94)
           (* (/ (* (* th th) -0.5) (sqrt 2.0)) (* a2_m a2_m))
           (/ (fma a2_m a2_m (* a1 a1)) (sqrt 2.0)))))
      a2_m = fabs(a2);
      assert(a1 < a2_m && a2_m < th);
      double code(double a1, double a2_m, double th) {
      	double t_1 = cos(th) / sqrt(2.0);
      	double tmp;
      	if (((t_1 * (a1 * a1)) + (t_1 * (a2_m * a2_m))) <= -1e-94) {
      		tmp = (((th * th) * -0.5) / sqrt(2.0)) * (a2_m * a2_m);
      	} else {
      		tmp = fma(a2_m, a2_m, (a1 * a1)) / sqrt(2.0);
      	}
      	return tmp;
      }
      
      a2_m = abs(a2)
      a1, a2_m, th = sort([a1, a2_m, th])
      function code(a1, a2_m, th)
      	t_1 = Float64(cos(th) / sqrt(2.0))
      	tmp = 0.0
      	if (Float64(Float64(t_1 * Float64(a1 * a1)) + Float64(t_1 * Float64(a2_m * a2_m))) <= -1e-94)
      		tmp = Float64(Float64(Float64(Float64(th * th) * -0.5) / sqrt(2.0)) * Float64(a2_m * a2_m));
      	else
      		tmp = Float64(fma(a2_m, a2_m, Float64(a1 * a1)) / sqrt(2.0));
      	end
      	return tmp
      end
      
      a2_m = N[Abs[a2], $MachinePrecision]
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      code[a1_, a2$95$m_, th_] := Block[{t$95$1 = N[(N[Cos[th], $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[N[(N[(t$95$1 * N[(a1 * a1), $MachinePrecision]), $MachinePrecision] + N[(t$95$1 * N[(a2$95$m * a2$95$m), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], -1e-94], N[(N[(N[(N[(th * th), $MachinePrecision] * -0.5), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision] * N[(a2$95$m * a2$95$m), $MachinePrecision]), $MachinePrecision], N[(N[(a2$95$m * a2$95$m + N[(a1 * a1), $MachinePrecision]), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]]]
      
      \begin{array}{l}
      a2_m = \left|a2\right|
      \\
      [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
      \\
      \begin{array}{l}
      t_1 := \frac{\cos th}{\sqrt{2}}\\
      \mathbf{if}\;t\_1 \cdot \left(a1 \cdot a1\right) + t\_1 \cdot \left(a2\_m \cdot a2\_m\right) \leq -1 \cdot 10^{-94}:\\
      \;\;\;\;\frac{\left(th \cdot th\right) \cdot -0.5}{\sqrt{2}} \cdot \left(a2\_m \cdot a2\_m\right)\\
      
      \mathbf{else}:\\
      \;\;\;\;\frac{\mathsf{fma}\left(a2\_m, a2\_m, a1 \cdot a1\right)}{\sqrt{2}}\\
      
      
      \end{array}
      \end{array}
      
      Derivation
      1. Split input into 2 regimes
      2. if (+.f64 (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a1 a1)) (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a2 a2))) < -9.9999999999999996e-95

        1. Initial program 99.5%

          \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        2. Taylor expanded in th around 0

          \[\leadsto \frac{\color{blue}{1 + \frac{-1}{2} \cdot {th}^{2}}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        3. Step-by-step derivation
          1. +-commutativeN/A

            \[\leadsto \frac{\frac{-1}{2} \cdot {th}^{2} + \color{blue}{1}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
          2. lower-fma.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, \color{blue}{{th}^{2}}, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
          3. unpow2N/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot \color{blue}{th}, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
          4. lower-*.f6471.6

            \[\leadsto \frac{\mathsf{fma}\left(-0.5, th \cdot \color{blue}{th}, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        4. Applied rewrites71.6%

          \[\leadsto \frac{\color{blue}{\mathsf{fma}\left(-0.5, th \cdot th, 1\right)}}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        5. Taylor expanded in th around 0

          \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\color{blue}{1 + \frac{-1}{2} \cdot {th}^{2}}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        6. Step-by-step derivation
          1. +-commutativeN/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\frac{-1}{2} \cdot {th}^{2} + \color{blue}{1}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
          2. lower-fma.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\mathsf{fma}\left(\frac{-1}{2}, \color{blue}{{th}^{2}}, 1\right)}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
          3. unpow2N/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot \color{blue}{th}, 1\right)}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
          4. lower-*.f6461.3

            \[\leadsto \frac{\mathsf{fma}\left(-0.5, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\mathsf{fma}\left(-0.5, th \cdot \color{blue}{th}, 1\right)}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        7. Applied rewrites61.3%

          \[\leadsto \frac{\mathsf{fma}\left(-0.5, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\color{blue}{\mathsf{fma}\left(-0.5, th \cdot th, 1\right)}}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        8. Step-by-step derivation
          1. lift-+.f64N/A

            \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
          2. lift-*.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \color{blue}{\left(a2 \cdot a2\right)} \]
          3. lift-*.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \color{blue}{\frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a2 \cdot a2\right)} \]
          4. pow2N/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} \]
          5. lift-*.f64N/A

            \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left(a1 \cdot a1\right)} + \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot {a2}^{2} \]
          6. lift-*.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \color{blue}{\left(a1 \cdot a1\right)} + \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot {a2}^{2} \]
          7. pow2N/A

            \[\leadsto \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \color{blue}{{a1}^{2}} + \frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot {a2}^{2} \]
          8. distribute-lft-outN/A

            \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left({a1}^{2} + {a2}^{2}\right)} \]
          9. lower-*.f64N/A

            \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(\frac{-1}{2}, th \cdot th, 1\right)}{\sqrt{2}} \cdot \left({a1}^{2} + {a2}^{2}\right)} \]
        9. Applied rewrites63.0%

          \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(th \cdot th, -0.5, 1\right)}{\sqrt{2}} \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right)} \]
        10. Taylor expanded in th around inf

          \[\leadsto \frac{\frac{-1}{2} \cdot \color{blue}{{th}^{2}}}{\sqrt{2}} \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right) \]
        11. Step-by-step derivation
          1. *-commutativeN/A

            \[\leadsto \frac{{th}^{2} \cdot \frac{-1}{2}}{\sqrt{2}} \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right) \]
          2. lower-*.f64N/A

            \[\leadsto \frac{{th}^{2} \cdot \frac{-1}{2}}{\sqrt{2}} \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right) \]
          3. pow2N/A

            \[\leadsto \frac{\left(th \cdot th\right) \cdot \frac{-1}{2}}{\sqrt{2}} \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right) \]
          4. lift-*.f6416.6

            \[\leadsto \frac{\left(th \cdot th\right) \cdot -0.5}{\sqrt{2}} \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right) \]
        12. Applied rewrites16.6%

          \[\leadsto \frac{\left(th \cdot th\right) \cdot \color{blue}{-0.5}}{\sqrt{2}} \cdot \mathsf{fma}\left(a1, a1, a2 \cdot a2\right) \]
        13. Taylor expanded in a1 around 0

          \[\leadsto \frac{\left(th \cdot th\right) \cdot \frac{-1}{2}}{\sqrt{2}} \cdot \color{blue}{{a2}^{2}} \]
        14. Step-by-step derivation
          1. pow2N/A

            \[\leadsto \frac{\left(th \cdot th\right) \cdot \frac{-1}{2}}{\sqrt{2}} \cdot \left(a2 \cdot \color{blue}{a2}\right) \]
          2. lift-*.f6415.4

            \[\leadsto \frac{\left(th \cdot th\right) \cdot -0.5}{\sqrt{2}} \cdot \left(a2 \cdot \color{blue}{a2}\right) \]
        15. Applied rewrites15.4%

          \[\leadsto \frac{\left(th \cdot th\right) \cdot -0.5}{\sqrt{2}} \cdot \color{blue}{\left(a2 \cdot a2\right)} \]

        if -9.9999999999999996e-95 < (+.f64 (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a1 a1)) (*.f64 (/.f64 (cos.f64 th) (sqrt.f64 #s(literal 2 binary64))) (*.f64 a2 a2)))

        1. Initial program 99.5%

          \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
        2. Taylor expanded in th around 0

          \[\leadsto \color{blue}{\frac{{a1}^{2}}{\sqrt{2}} + \frac{{a2}^{2}}{\sqrt{2}}} \]
        3. Step-by-step derivation
          1. +-commutativeN/A

            \[\leadsto \frac{{a2}^{2}}{\sqrt{2}} + \color{blue}{\frac{{a1}^{2}}{\sqrt{2}}} \]
          2. div-add-revN/A

            \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
          3. lower-/.f64N/A

            \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
          4. pow2N/A

            \[\leadsto \frac{a2 \cdot a2 + {a1}^{2}}{\sqrt{2}} \]
          5. lower-fma.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(a2, a2, {a1}^{2}\right)}{\sqrt{\color{blue}{2}}} \]
          6. pow2N/A

            \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
          7. lift-*.f64N/A

            \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
          8. lift-sqrt.f6466.5

            \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
        4. Applied rewrites66.5%

          \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}}} \]
      3. Recombined 2 regimes into one program.
      4. Add Preprocessing

      Alternative 11: 66.5% accurate, 6.4× speedup?

      \[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \frac{\mathsf{fma}\left(a2\_m, a2\_m, a1 \cdot a1\right)}{\sqrt{2}} \end{array} \]
      a2_m = (fabs.f64 a2)
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      (FPCore (a1 a2_m th)
       :precision binary64
       (/ (fma a2_m a2_m (* a1 a1)) (sqrt 2.0)))
      a2_m = fabs(a2);
      assert(a1 < a2_m && a2_m < th);
      double code(double a1, double a2_m, double th) {
      	return fma(a2_m, a2_m, (a1 * a1)) / sqrt(2.0);
      }
      
      a2_m = abs(a2)
      a1, a2_m, th = sort([a1, a2_m, th])
      function code(a1, a2_m, th)
      	return Float64(fma(a2_m, a2_m, Float64(a1 * a1)) / sqrt(2.0))
      end
      
      a2_m = N[Abs[a2], $MachinePrecision]
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      code[a1_, a2$95$m_, th_] := N[(N[(a2$95$m * a2$95$m + N[(a1 * a1), $MachinePrecision]), $MachinePrecision] / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]
      
      \begin{array}{l}
      a2_m = \left|a2\right|
      \\
      [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
      \\
      \frac{\mathsf{fma}\left(a2\_m, a2\_m, a1 \cdot a1\right)}{\sqrt{2}}
      \end{array}
      
      Derivation
      1. Initial program 99.5%

        \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      2. Taylor expanded in th around 0

        \[\leadsto \color{blue}{\frac{{a1}^{2}}{\sqrt{2}} + \frac{{a2}^{2}}{\sqrt{2}}} \]
      3. Step-by-step derivation
        1. +-commutativeN/A

          \[\leadsto \frac{{a2}^{2}}{\sqrt{2}} + \color{blue}{\frac{{a1}^{2}}{\sqrt{2}}} \]
        2. div-add-revN/A

          \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
        3. lower-/.f64N/A

          \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
        4. pow2N/A

          \[\leadsto \frac{a2 \cdot a2 + {a1}^{2}}{\sqrt{2}} \]
        5. lower-fma.f64N/A

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, {a1}^{2}\right)}{\sqrt{\color{blue}{2}}} \]
        6. pow2N/A

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
        7. lift-*.f64N/A

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
        8. lift-sqrt.f6466.5

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
      4. Applied rewrites66.5%

        \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}}} \]
      5. Add Preprocessing

      Alternative 12: 53.1% accurate, 9.9× speedup?

      \[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ \frac{a2\_m}{\sqrt{2}} \cdot a2\_m \end{array} \]
      a2_m = (fabs.f64 a2)
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      (FPCore (a1 a2_m th) :precision binary64 (* (/ a2_m (sqrt 2.0)) a2_m))
      a2_m = fabs(a2);
      assert(a1 < a2_m && a2_m < th);
      double code(double a1, double a2_m, double th) {
      	return (a2_m / sqrt(2.0)) * a2_m;
      }
      
      a2_m =     private
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      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(a1, a2_m, th)
      use fmin_fmax_functions
          real(8), intent (in) :: a1
          real(8), intent (in) :: a2_m
          real(8), intent (in) :: th
          code = (a2_m / sqrt(2.0d0)) * a2_m
      end function
      
      a2_m = Math.abs(a2);
      assert a1 < a2_m && a2_m < th;
      public static double code(double a1, double a2_m, double th) {
      	return (a2_m / Math.sqrt(2.0)) * a2_m;
      }
      
      a2_m = math.fabs(a2)
      [a1, a2_m, th] = sort([a1, a2_m, th])
      def code(a1, a2_m, th):
      	return (a2_m / math.sqrt(2.0)) * a2_m
      
      a2_m = abs(a2)
      a1, a2_m, th = sort([a1, a2_m, th])
      function code(a1, a2_m, th)
      	return Float64(Float64(a2_m / sqrt(2.0)) * a2_m)
      end
      
      a2_m = abs(a2);
      a1, a2_m, th = num2cell(sort([a1, a2_m, th])){:}
      function tmp = code(a1, a2_m, th)
      	tmp = (a2_m / sqrt(2.0)) * a2_m;
      end
      
      a2_m = N[Abs[a2], $MachinePrecision]
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      code[a1_, a2$95$m_, th_] := N[(N[(a2$95$m / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision] * a2$95$m), $MachinePrecision]
      
      \begin{array}{l}
      a2_m = \left|a2\right|
      \\
      [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
      \\
      \frac{a2\_m}{\sqrt{2}} \cdot a2\_m
      \end{array}
      
      Derivation
      1. Initial program 99.5%

        \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      2. Taylor expanded in th around 0

        \[\leadsto \color{blue}{\frac{{a1}^{2}}{\sqrt{2}} + \frac{{a2}^{2}}{\sqrt{2}}} \]
      3. Step-by-step derivation
        1. +-commutativeN/A

          \[\leadsto \frac{{a2}^{2}}{\sqrt{2}} + \color{blue}{\frac{{a1}^{2}}{\sqrt{2}}} \]
        2. div-add-revN/A

          \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
        3. lower-/.f64N/A

          \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
        4. pow2N/A

          \[\leadsto \frac{a2 \cdot a2 + {a1}^{2}}{\sqrt{2}} \]
        5. lower-fma.f64N/A

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, {a1}^{2}\right)}{\sqrt{\color{blue}{2}}} \]
        6. pow2N/A

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
        7. lift-*.f64N/A

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
        8. lift-sqrt.f6466.5

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
      4. Applied rewrites66.5%

        \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}}} \]
      5. Taylor expanded in a1 around 0

        \[\leadsto \frac{{a2}^{2}}{\color{blue}{\sqrt{2}}} \]
      6. Step-by-step derivation
        1. pow2N/A

          \[\leadsto \frac{a2 \cdot a2}{\sqrt{2}} \]
        2. associate-*r/N/A

          \[\leadsto a2 \cdot \frac{a2}{\color{blue}{\sqrt{2}}} \]
        3. *-commutativeN/A

          \[\leadsto \frac{a2}{\sqrt{2}} \cdot a2 \]
        4. lower-*.f64N/A

          \[\leadsto \frac{a2}{\sqrt{2}} \cdot a2 \]
        5. lift-sqrt.f64N/A

          \[\leadsto \frac{a2}{\sqrt{2}} \cdot a2 \]
        6. lift-/.f6453.1

          \[\leadsto \frac{a2}{\sqrt{2}} \cdot a2 \]
      7. Applied rewrites53.1%

        \[\leadsto \frac{a2}{\sqrt{2}} \cdot \color{blue}{a2} \]
      8. Add Preprocessing

      Alternative 13: 27.1% accurate, 9.9× speedup?

      \[\begin{array}{l} a2_m = \left|a2\right| \\ [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\ \\ a1 \cdot \frac{a1}{\sqrt{2}} \end{array} \]
      a2_m = (fabs.f64 a2)
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      (FPCore (a1 a2_m th) :precision binary64 (* a1 (/ a1 (sqrt 2.0))))
      a2_m = fabs(a2);
      assert(a1 < a2_m && a2_m < th);
      double code(double a1, double a2_m, double th) {
      	return a1 * (a1 / sqrt(2.0));
      }
      
      a2_m =     private
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      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(a1, a2_m, th)
      use fmin_fmax_functions
          real(8), intent (in) :: a1
          real(8), intent (in) :: a2_m
          real(8), intent (in) :: th
          code = a1 * (a1 / sqrt(2.0d0))
      end function
      
      a2_m = Math.abs(a2);
      assert a1 < a2_m && a2_m < th;
      public static double code(double a1, double a2_m, double th) {
      	return a1 * (a1 / Math.sqrt(2.0));
      }
      
      a2_m = math.fabs(a2)
      [a1, a2_m, th] = sort([a1, a2_m, th])
      def code(a1, a2_m, th):
      	return a1 * (a1 / math.sqrt(2.0))
      
      a2_m = abs(a2)
      a1, a2_m, th = sort([a1, a2_m, th])
      function code(a1, a2_m, th)
      	return Float64(a1 * Float64(a1 / sqrt(2.0)))
      end
      
      a2_m = abs(a2);
      a1, a2_m, th = num2cell(sort([a1, a2_m, th])){:}
      function tmp = code(a1, a2_m, th)
      	tmp = a1 * (a1 / sqrt(2.0));
      end
      
      a2_m = N[Abs[a2], $MachinePrecision]
      NOTE: a1, a2_m, and th should be sorted in increasing order before calling this function.
      code[a1_, a2$95$m_, th_] := N[(a1 * N[(a1 / N[Sqrt[2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
      
      \begin{array}{l}
      a2_m = \left|a2\right|
      \\
      [a1, a2_m, th] = \mathsf{sort}([a1, a2_m, th])\\
      \\
      a1 \cdot \frac{a1}{\sqrt{2}}
      \end{array}
      
      Derivation
      1. Initial program 99.5%

        \[\frac{\cos th}{\sqrt{2}} \cdot \left(a1 \cdot a1\right) + \frac{\cos th}{\sqrt{2}} \cdot \left(a2 \cdot a2\right) \]
      2. Taylor expanded in th around 0

        \[\leadsto \color{blue}{\frac{{a1}^{2}}{\sqrt{2}} + \frac{{a2}^{2}}{\sqrt{2}}} \]
      3. Step-by-step derivation
        1. +-commutativeN/A

          \[\leadsto \frac{{a2}^{2}}{\sqrt{2}} + \color{blue}{\frac{{a1}^{2}}{\sqrt{2}}} \]
        2. div-add-revN/A

          \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
        3. lower-/.f64N/A

          \[\leadsto \frac{{a2}^{2} + {a1}^{2}}{\color{blue}{\sqrt{2}}} \]
        4. pow2N/A

          \[\leadsto \frac{a2 \cdot a2 + {a1}^{2}}{\sqrt{2}} \]
        5. lower-fma.f64N/A

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, {a1}^{2}\right)}{\sqrt{\color{blue}{2}}} \]
        6. pow2N/A

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
        7. lift-*.f64N/A

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
        8. lift-sqrt.f6466.5

          \[\leadsto \frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}} \]
      4. Applied rewrites66.5%

        \[\leadsto \color{blue}{\frac{\mathsf{fma}\left(a2, a2, a1 \cdot a1\right)}{\sqrt{2}}} \]
      5. Taylor expanded in a1 around inf

        \[\leadsto \frac{{a1}^{2}}{\color{blue}{\sqrt{2}}} \]
      6. Step-by-step derivation
        1. lower-/.f64N/A

          \[\leadsto \frac{{a1}^{2}}{\sqrt{2}} \]
        2. pow2N/A

          \[\leadsto \frac{a1 \cdot a1}{\sqrt{2}} \]
        3. lift-*.f64N/A

          \[\leadsto \frac{a1 \cdot a1}{\sqrt{2}} \]
        4. lift-sqrt.f6427.1

          \[\leadsto \frac{a1 \cdot a1}{\sqrt{2}} \]
      7. Applied rewrites27.1%

        \[\leadsto \frac{a1 \cdot a1}{\color{blue}{\sqrt{2}}} \]
      8. Step-by-step derivation
        1. lift-*.f64N/A

          \[\leadsto \frac{a1 \cdot a1}{\sqrt{2}} \]
        2. lift-/.f64N/A

          \[\leadsto \frac{a1 \cdot a1}{\sqrt{2}} \]
        3. lift-sqrt.f64N/A

          \[\leadsto \frac{a1 \cdot a1}{\sqrt{2}} \]
        4. associate-/l*N/A

          \[\leadsto a1 \cdot \frac{a1}{\color{blue}{\sqrt{2}}} \]
        5. lower-*.f64N/A

          \[\leadsto a1 \cdot \frac{a1}{\color{blue}{\sqrt{2}}} \]
        6. lift-sqrt.f64N/A

          \[\leadsto a1 \cdot \frac{a1}{\sqrt{2}} \]
        7. lift-/.f6427.1

          \[\leadsto a1 \cdot \frac{a1}{\sqrt{2}} \]
      9. Applied rewrites27.1%

        \[\leadsto a1 \cdot \color{blue}{\frac{a1}{\sqrt{2}}} \]
      10. Add Preprocessing

      Reproduce

      ?
      herbie shell --seed 2025142 
      (FPCore (a1 a2 th)
        :name "Migdal et al, Equation (64)"
        :precision binary64
        (+ (* (/ (cos th) (sqrt 2.0)) (* a1 a1)) (* (/ (cos th) (sqrt 2.0)) (* a2 a2))))