Toniolo and Linder, Equation (3a)

Percentage Accurate: 98.6% → 99.5%

Time: 8.6s

Alternatives: 6

Speedup: 2.1×

Specification

Math

\[\begin{array}{l} \\ \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \end{array} \]

FPCore

(FPCore (l Om kx ky)
 :precision binary64
 (sqrt
  (*
   (/ 1.0 2.0)
   (+
    1.0
    (/
     1.0
     (sqrt
      (+
       1.0
       (*
        (pow (/ (* 2.0 l) Om) 2.0)
        (+ (pow (sin kx) 2.0) (pow (sin ky) 2.0))))))))))

C

double code(double l, double Om, double kx, double ky) {
	return sqrt(((1.0 / 2.0) * (1.0 + (1.0 / sqrt((1.0 + (pow(((2.0 * l) / Om), 2.0) * (pow(sin(kx), 2.0) + pow(sin(ky), 2.0)))))))));
}

Fortran

real(8) function code(l, om, kx, ky)
    real(8), intent (in) :: l
    real(8), intent (in) :: om
    real(8), intent (in) :: kx
    real(8), intent (in) :: ky
    code = sqrt(((1.0d0 / 2.0d0) * (1.0d0 + (1.0d0 / sqrt((1.0d0 + ((((2.0d0 * l) / om) ** 2.0d0) * ((sin(kx) ** 2.0d0) + (sin(ky) ** 2.0d0)))))))))
end function

Java

public static double code(double l, double Om, double kx, double ky) {
	return Math.sqrt(((1.0 / 2.0) * (1.0 + (1.0 / Math.sqrt((1.0 + (Math.pow(((2.0 * l) / Om), 2.0) * (Math.pow(Math.sin(kx), 2.0) + Math.pow(Math.sin(ky), 2.0)))))))));
}

Python

def code(l, Om, kx, ky):
	return math.sqrt(((1.0 / 2.0) * (1.0 + (1.0 / math.sqrt((1.0 + (math.pow(((2.0 * l) / Om), 2.0) * (math.pow(math.sin(kx), 2.0) + math.pow(math.sin(ky), 2.0)))))))))

Julia

function code(l, Om, kx, ky)
	return sqrt(Float64(Float64(1.0 / 2.0) * Float64(1.0 + Float64(1.0 / sqrt(Float64(1.0 + Float64((Float64(Float64(2.0 * l) / Om) ^ 2.0) * Float64((sin(kx) ^ 2.0) + (sin(ky) ^ 2.0)))))))))
end

MATLAB

function tmp = code(l, Om, kx, ky)
	tmp = sqrt(((1.0 / 2.0) * (1.0 + (1.0 / sqrt((1.0 + ((((2.0 * l) / Om) ^ 2.0) * ((sin(kx) ^ 2.0) + (sin(ky) ^ 2.0)))))))));
end

Wolfram

code[l_, Om_, kx_, ky_] := N[Sqrt[N[(N[(1.0 / 2.0), $MachinePrecision] * N[(1.0 + N[(1.0 / N[Sqrt[N[(1.0 + N[(N[Power[N[(N[(2.0 * l), $MachinePrecision] / Om), $MachinePrecision], 2.0], $MachinePrecision] * N[(N[Power[N[Sin[kx], $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[Sin[ky], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]

Initial Program: 98.6% accurate, 1.0× speedup

Math

\[\begin{array}{l} \\ \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \end{array} \]

FPCore

(FPCore (l Om kx ky)
 :precision binary64
 (sqrt
  (*
   (/ 1.0 2.0)
   (+
    1.0
    (/
     1.0
     (sqrt
      (+
       1.0
       (*
        (pow (/ (* 2.0 l) Om) 2.0)
        (+ (pow (sin kx) 2.0) (pow (sin ky) 2.0))))))))))

C

double code(double l, double Om, double kx, double ky) {
	return sqrt(((1.0 / 2.0) * (1.0 + (1.0 / sqrt((1.0 + (pow(((2.0 * l) / Om), 2.0) * (pow(sin(kx), 2.0) + pow(sin(ky), 2.0)))))))));
}

Fortran

real(8) function code(l, om, kx, ky)
    real(8), intent (in) :: l
    real(8), intent (in) :: om
    real(8), intent (in) :: kx
    real(8), intent (in) :: ky
    code = sqrt(((1.0d0 / 2.0d0) * (1.0d0 + (1.0d0 / sqrt((1.0d0 + ((((2.0d0 * l) / om) ** 2.0d0) * ((sin(kx) ** 2.0d0) + (sin(ky) ** 2.0d0)))))))))
end function

Java

public static double code(double l, double Om, double kx, double ky) {
	return Math.sqrt(((1.0 / 2.0) * (1.0 + (1.0 / Math.sqrt((1.0 + (Math.pow(((2.0 * l) / Om), 2.0) * (Math.pow(Math.sin(kx), 2.0) + Math.pow(Math.sin(ky), 2.0)))))))));
}

Python

def code(l, Om, kx, ky):
	return math.sqrt(((1.0 / 2.0) * (1.0 + (1.0 / math.sqrt((1.0 + (math.pow(((2.0 * l) / Om), 2.0) * (math.pow(math.sin(kx), 2.0) + math.pow(math.sin(ky), 2.0)))))))))

Julia

function code(l, Om, kx, ky)
	return sqrt(Float64(Float64(1.0 / 2.0) * Float64(1.0 + Float64(1.0 / sqrt(Float64(1.0 + Float64((Float64(Float64(2.0 * l) / Om) ^ 2.0) * Float64((sin(kx) ^ 2.0) + (sin(ky) ^ 2.0)))))))))
end

MATLAB

function tmp = code(l, Om, kx, ky)
	tmp = sqrt(((1.0 / 2.0) * (1.0 + (1.0 / sqrt((1.0 + ((((2.0 * l) / Om) ^ 2.0) * ((sin(kx) ^ 2.0) + (sin(ky) ^ 2.0)))))))));
end

Wolfram

code[l_, Om_, kx_, ky_] := N[Sqrt[N[(N[(1.0 / 2.0), $MachinePrecision] * N[(1.0 + N[(1.0 / N[Sqrt[N[(1.0 + N[(N[Power[N[(N[(2.0 * l), $MachinePrecision] / Om), $MachinePrecision], 2.0], $MachinePrecision] * N[(N[Power[N[Sin[kx], $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[Sin[ky], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]

Alternative 1: 99.5% accurate, 2.1× speedup

Math

\[\begin{array}{l} ky_m = \left|ky\right| \\ kx_m = \left|kx\right| \\ [l, Om, kx_m, ky_m] = \mathsf{sort}([l, Om, kx_m, ky_m])\\ \\ \sqrt{\left(\sqrt{\frac{1}{{\left(\frac{\ell \cdot 2}{Om} \cdot \sin ky\_m\right)}^{2} + 1}} + 1\right) \cdot \frac{1}{2}} \end{array} \]

FPCore

ky_m = (fabs.f64 ky)
kx_m = (fabs.f64 kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
(FPCore (l Om kx_m ky_m)
 :precision binary64
 (sqrt
  (*
   (+ (sqrt (/ 1.0 (+ (pow (* (/ (* l 2.0) Om) (sin ky_m)) 2.0) 1.0))) 1.0)
   (/ 1.0 2.0))))

C

ky_m = fabs(ky);
kx_m = fabs(kx);
assert(l < Om && Om < kx_m && kx_m < ky_m);
double code(double l, double Om, double kx_m, double ky_m) {
	return sqrt(((sqrt((1.0 / (pow((((l * 2.0) / Om) * sin(ky_m)), 2.0) + 1.0))) + 1.0) * (1.0 / 2.0)));
}

Fortran

ky_m = abs(ky)
kx_m = abs(kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
real(8) function code(l, om, kx_m, ky_m)
    real(8), intent (in) :: l
    real(8), intent (in) :: om
    real(8), intent (in) :: kx_m
    real(8), intent (in) :: ky_m
    code = sqrt(((sqrt((1.0d0 / (((((l * 2.0d0) / om) * sin(ky_m)) ** 2.0d0) + 1.0d0))) + 1.0d0) * (1.0d0 / 2.0d0)))
end function

Java

ky_m = Math.abs(ky);
kx_m = Math.abs(kx);
assert l < Om && Om < kx_m && kx_m < ky_m;
public static double code(double l, double Om, double kx_m, double ky_m) {
	return Math.sqrt(((Math.sqrt((1.0 / (Math.pow((((l * 2.0) / Om) * Math.sin(ky_m)), 2.0) + 1.0))) + 1.0) * (1.0 / 2.0)));
}

Python

ky_m = math.fabs(ky)
kx_m = math.fabs(kx)
[l, Om, kx_m, ky_m] = sort([l, Om, kx_m, ky_m])
def code(l, Om, kx_m, ky_m):
	return math.sqrt(((math.sqrt((1.0 / (math.pow((((l * 2.0) / Om) * math.sin(ky_m)), 2.0) + 1.0))) + 1.0) * (1.0 / 2.0)))

Julia

ky_m = abs(ky)
kx_m = abs(kx)
l, Om, kx_m, ky_m = sort([l, Om, kx_m, ky_m])
function code(l, Om, kx_m, ky_m)
	return sqrt(Float64(Float64(sqrt(Float64(1.0 / Float64((Float64(Float64(Float64(l * 2.0) / Om) * sin(ky_m)) ^ 2.0) + 1.0))) + 1.0) * Float64(1.0 / 2.0)))
end

MATLAB

ky_m = abs(ky);
kx_m = abs(kx);
l, Om, kx_m, ky_m = num2cell(sort([l, Om, kx_m, ky_m])){:}
function tmp = code(l, Om, kx_m, ky_m)
	tmp = sqrt(((sqrt((1.0 / (((((l * 2.0) / Om) * sin(ky_m)) ^ 2.0) + 1.0))) + 1.0) * (1.0 / 2.0)));
end

Wolfram

ky_m = N[Abs[ky], $MachinePrecision]
kx_m = N[Abs[kx], $MachinePrecision]
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
code[l_, Om_, kx$95$m_, ky$95$m_] := N[Sqrt[N[(N[(N[Sqrt[N[(1.0 / N[(N[Power[N[(N[(N[(l * 2.0), $MachinePrecision] / Om), $MachinePrecision] * N[Sin[ky$95$m], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + 1.0), $MachinePrecision] * N[(1.0 / 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]

Derivation

1. Initial program 99.2%

   \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
2. Add Preprocessing

3. Taylor expanded in kx around 0

   \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]
4. Step-by-step derivation

   1. lower-sqrt.f64 N/A

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]

   2. lower-/.f64 N/A

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\color{blue}{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]

   3. +-commutative N/A

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}} + 1}}}\right)} \]

   4. associate-/l* N/A

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{4 \cdot \color{blue}{\left({\ell}^{2} \cdot \frac{{\sin ky}^{2}}{{Om}^{2}}\right)} + 1}}\right)} \]

   5. associate-*r* N/A

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{\left(4 \cdot {\ell}^{2}\right) \cdot \frac{{\sin ky}^{2}}{{Om}^{2}}} + 1}}\right)} \]

   6. lower-fma.f64 N/A

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{\mathsf{fma}\left(4 \cdot {\ell}^{2}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}}\right)} \]

   7. lower-*.f64 N/A

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(\color{blue}{4 \cdot {\ell}^{2}}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

   8. unpow2 N/A

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \color{blue}{\left(\ell \cdot \ell\right)}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

   9. lower-*.f64 N/A

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \color{blue}{\left(\ell \cdot \ell\right)}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

   10. lower-/.f64 N/A

       \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \color{blue}{\frac{{\sin ky}^{2}}{{Om}^{2}}}, 1\right)}}\right)} \]

   11. lower-pow.f64 N/A

       \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{\color{blue}{{\sin ky}^{2}}}{{Om}^{2}}, 1\right)}}\right)} \]

   12. lower-sin.f64 N/A

       \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\color{blue}{\sin ky}}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

   13. unpow2 N/A

       \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{\color{blue}{Om \cdot Om}}, 1\right)}}\right)} \]

   14. lower-*.f64 81.3

       \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{\color{blue}{Om \cdot Om}}, 1\right)}}\right)} \]

5. Applied rewrites 81.3%

   \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{Om \cdot Om}, 1\right)}}}\right)} \]
6. Step-by-step derivation

7. Applied rewrites 93.0%

   \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{{\left(\sin ky \cdot \frac{\ell \cdot 2}{Om}\right)}^{2} + 1}}\right)} \]

8. Final simplification 93.0%

   \[\leadsto \sqrt{\left(\sqrt{\frac{1}{{\left(\frac{\ell \cdot 2}{Om} \cdot \sin ky\right)}^{2} + 1}} + 1\right) \cdot \frac{1}{2}} \]
9. Add Preprocessing

Alternative 2: 98.4% accurate, 0.8× speedup

Math

\[\begin{array}{l} ky_m = \left|ky\right| \\ kx_m = \left|kx\right| \\ [l, Om, kx_m, ky_m] = \mathsf{sort}([l, Om, kx_m, ky_m])\\ \\ \begin{array}{l} \mathbf{if}\;\left({\sin ky\_m}^{2} + {\sin kx\_m}^{2}\right) \cdot {\left(\frac{\ell \cdot 2}{Om}\right)}^{2} \leq 0.4:\\ \;\;\;\;\sqrt{0.5 + 0.5}\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\left(\frac{Om}{\sin ky\_m \cdot \ell} \cdot 0.5 + 1\right) \cdot \frac{1}{2}}\\ \end{array} \end{array} \]

FPCore

ky_m = (fabs.f64 ky)
kx_m = (fabs.f64 kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
(FPCore (l Om kx_m ky_m)
 :precision binary64
 (if (<=
      (*
       (+ (pow (sin ky_m) 2.0) (pow (sin kx_m) 2.0))
       (pow (/ (* l 2.0) Om) 2.0))
      0.4)
   (sqrt (+ 0.5 0.5))
   (sqrt (* (+ (* (/ Om (* (sin ky_m) l)) 0.5) 1.0) (/ 1.0 2.0)))))

C

ky_m = fabs(ky);
kx_m = fabs(kx);
assert(l < Om && Om < kx_m && kx_m < ky_m);
double code(double l, double Om, double kx_m, double ky_m) {
	double tmp;
	if (((pow(sin(ky_m), 2.0) + pow(sin(kx_m), 2.0)) * pow(((l * 2.0) / Om), 2.0)) <= 0.4) {
		tmp = sqrt((0.5 + 0.5));
	} else {
		tmp = sqrt(((((Om / (sin(ky_m) * l)) * 0.5) + 1.0) * (1.0 / 2.0)));
	}
	return tmp;
}

Fortran

ky_m = abs(ky)
kx_m = abs(kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
real(8) function code(l, om, kx_m, ky_m)
    real(8), intent (in) :: l
    real(8), intent (in) :: om
    real(8), intent (in) :: kx_m
    real(8), intent (in) :: ky_m
    real(8) :: tmp
    if ((((sin(ky_m) ** 2.0d0) + (sin(kx_m) ** 2.0d0)) * (((l * 2.0d0) / om) ** 2.0d0)) <= 0.4d0) then
        tmp = sqrt((0.5d0 + 0.5d0))
    else
        tmp = sqrt(((((om / (sin(ky_m) * l)) * 0.5d0) + 1.0d0) * (1.0d0 / 2.0d0)))
    end if
    code = tmp
end function

Java

ky_m = Math.abs(ky);
kx_m = Math.abs(kx);
assert l < Om && Om < kx_m && kx_m < ky_m;
public static double code(double l, double Om, double kx_m, double ky_m) {
	double tmp;
	if (((Math.pow(Math.sin(ky_m), 2.0) + Math.pow(Math.sin(kx_m), 2.0)) * Math.pow(((l * 2.0) / Om), 2.0)) <= 0.4) {
		tmp = Math.sqrt((0.5 + 0.5));
	} else {
		tmp = Math.sqrt(((((Om / (Math.sin(ky_m) * l)) * 0.5) + 1.0) * (1.0 / 2.0)));
	}
	return tmp;
}

Python

ky_m = math.fabs(ky)
kx_m = math.fabs(kx)
[l, Om, kx_m, ky_m] = sort([l, Om, kx_m, ky_m])
def code(l, Om, kx_m, ky_m):
	tmp = 0
	if ((math.pow(math.sin(ky_m), 2.0) + math.pow(math.sin(kx_m), 2.0)) * math.pow(((l * 2.0) / Om), 2.0)) <= 0.4:
		tmp = math.sqrt((0.5 + 0.5))
	else:
		tmp = math.sqrt(((((Om / (math.sin(ky_m) * l)) * 0.5) + 1.0) * (1.0 / 2.0)))
	return tmp

Julia

ky_m = abs(ky)
kx_m = abs(kx)
l, Om, kx_m, ky_m = sort([l, Om, kx_m, ky_m])
function code(l, Om, kx_m, ky_m)
	tmp = 0.0
	if (Float64(Float64((sin(ky_m) ^ 2.0) + (sin(kx_m) ^ 2.0)) * (Float64(Float64(l * 2.0) / Om) ^ 2.0)) <= 0.4)
		tmp = sqrt(Float64(0.5 + 0.5));
	else
		tmp = sqrt(Float64(Float64(Float64(Float64(Om / Float64(sin(ky_m) * l)) * 0.5) + 1.0) * Float64(1.0 / 2.0)));
	end
	return tmp
end

MATLAB

ky_m = abs(ky);
kx_m = abs(kx);
l, Om, kx_m, ky_m = num2cell(sort([l, Om, kx_m, ky_m])){:}
function tmp_2 = code(l, Om, kx_m, ky_m)
	tmp = 0.0;
	if ((((sin(ky_m) ^ 2.0) + (sin(kx_m) ^ 2.0)) * (((l * 2.0) / Om) ^ 2.0)) <= 0.4)
		tmp = sqrt((0.5 + 0.5));
	else
		tmp = sqrt(((((Om / (sin(ky_m) * l)) * 0.5) + 1.0) * (1.0 / 2.0)));
	end
	tmp_2 = tmp;
end

Wolfram

ky_m = N[Abs[ky], $MachinePrecision]
kx_m = N[Abs[kx], $MachinePrecision]
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
code[l_, Om_, kx$95$m_, ky$95$m_] := If[LessEqual[N[(N[(N[Power[N[Sin[ky$95$m], $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[Sin[kx$95$m], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] * N[Power[N[(N[(l * 2.0), $MachinePrecision] / Om), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision], 0.4], N[Sqrt[N[(0.5 + 0.5), $MachinePrecision]], $MachinePrecision], N[Sqrt[N[(N[(N[(N[(Om / N[(N[Sin[ky$95$m], $MachinePrecision] * l), $MachinePrecision]), $MachinePrecision] * 0.5), $MachinePrecision] + 1.0), $MachinePrecision] * N[(1.0 / 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Derivation

1. Split input into 2 regimes

2. if (*.f64 (pow.f64 (/.f64 (*.f64 #s(literal 2 binary64) l) Om) #s(literal 2 binary64)) (+.f64 (pow.f64 (sin.f64 kx) #s(literal 2 binary64)) (pow.f64 (sin.f64 ky) #s(literal 2 binary64)))) < 0.40000000000000002

   1. Initial program 100.0%

      \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
   2. Add Preprocessing

   3. Taylor expanded in l around 0

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
   4. Step-by-step derivation

   5. Applied rewrites 98.0%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
   6. Step-by-step derivation

      1. lift-*.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2} \cdot \left(1 + \frac{1}{1}\right)}} \]

      2. lift-/.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} \cdot \left(1 + \frac{1}{1}\right)} \]

      3. metadata-eval N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} \cdot \left(1 + \frac{1}{1}\right)} \]

      4. lift-+.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \color{blue}{\left(1 + \frac{1}{1}\right)}} \]

      5. +-commutative N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \color{blue}{\left(\frac{1}{1} + 1\right)}} \]

      6. distribute-rgt-in N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{1} \cdot \frac{1}{2} + 1 \cdot \frac{1}{2}}} \]

      7. metadata-eval N/A

         \[\leadsto \sqrt{\frac{1}{1} \cdot \frac{1}{2} + \color{blue}{\frac{1}{2}}} \]

      8. lower-+.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{1} \cdot \frac{1}{2} + \frac{1}{2}}} \]

   7. Applied rewrites 98.0%

      \[\leadsto \color{blue}{\sqrt{\frac{0.5}{1} + 0.5}} \]

   8. Taylor expanded in l around 0

      \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} + \frac{1}{2}} \]
   9. Step-by-step derivation

   10. Applied rewrites 98.0%

       \[\leadsto \sqrt{\color{blue}{0.5} + 0.5} \]

   if 0.40000000000000002 < (*.f64 (pow.f64 (/.f64 (*.f64 #s(literal 2 binary64) l) Om) #s(literal 2 binary64)) (+.f64 (pow.f64 (sin.f64 kx) #s(literal 2 binary64)) (pow.f64 (sin.f64 ky) #s(literal 2 binary64))))

   1. Initial program 98.1%

      \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
   2. Add Preprocessing

   3. Taylor expanded in kx around 0

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]
   4. Step-by-step derivation

      1. lower-sqrt.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]

      2. lower-/.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\color{blue}{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]

      3. +-commutative N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}} + 1}}}\right)} \]

      4. associate-/l* N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{4 \cdot \color{blue}{\left({\ell}^{2} \cdot \frac{{\sin ky}^{2}}{{Om}^{2}}\right)} + 1}}\right)} \]

      5. associate-*r* N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{\left(4 \cdot {\ell}^{2}\right) \cdot \frac{{\sin ky}^{2}}{{Om}^{2}}} + 1}}\right)} \]

      6. lower-fma.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{\mathsf{fma}\left(4 \cdot {\ell}^{2}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}}\right)} \]

      7. lower-*.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(\color{blue}{4 \cdot {\ell}^{2}}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      8. unpow2 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \color{blue}{\left(\ell \cdot \ell\right)}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      9. lower-*.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \color{blue}{\left(\ell \cdot \ell\right)}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      10. lower-/.f64 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \color{blue}{\frac{{\sin ky}^{2}}{{Om}^{2}}}, 1\right)}}\right)} \]

      11. lower-pow.f64 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{\color{blue}{{\sin ky}^{2}}}{{Om}^{2}}, 1\right)}}\right)} \]

      12. lower-sin.f64 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\color{blue}{\sin ky}}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      13. unpow2 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{\color{blue}{Om \cdot Om}}, 1\right)}}\right)} \]

      14. lower-*.f64 69.7

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{\color{blue}{Om \cdot Om}}, 1\right)}}\right)} \]

   5. Applied rewrites 69.7%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{Om \cdot Om}, 1\right)}}}\right)} \]

   6. Taylor expanded in l around inf

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{2} \cdot \color{blue}{\frac{Om}{\ell \cdot \sin ky}}\right)} \]
   7. Step-by-step derivation

   8. Applied rewrites 80.6%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{Om}{\sin ky \cdot \ell} \cdot \color{blue}{0.5}\right)} \]
3. Recombined 2 regimes into one program.

4. Final simplification 90.7%

   \[\leadsto \begin{array}{l} \mathbf{if}\;\left({\sin ky}^{2} + {\sin kx}^{2}\right) \cdot {\left(\frac{\ell \cdot 2}{Om}\right)}^{2} \leq 0.4:\\ \;\;\;\;\sqrt{0.5 + 0.5}\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\left(\frac{Om}{\sin ky \cdot \ell} \cdot 0.5 + 1\right) \cdot \frac{1}{2}}\\ \end{array} \]
5. Add Preprocessing

Alternative 3: 98.4% accurate, 0.8× speedup

Math

\[\begin{array}{l} ky_m = \left|ky\right| \\ kx_m = \left|kx\right| \\ [l, Om, kx_m, ky_m] = \mathsf{sort}([l, Om, kx_m, ky_m])\\ \\ \begin{array}{l} \mathbf{if}\;\left({\sin ky\_m}^{2} + {\sin kx\_m}^{2}\right) \cdot {\left(\frac{\ell \cdot 2}{Om}\right)}^{2} \leq 2:\\ \;\;\;\;\sqrt{0.5 + 0.5}\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\left(-0.5 \cdot \frac{Om}{\sin ky\_m \cdot \ell} + 1\right) \cdot \frac{1}{2}}\\ \end{array} \end{array} \]

FPCore

ky_m = (fabs.f64 ky)
kx_m = (fabs.f64 kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
(FPCore (l Om kx_m ky_m)
 :precision binary64
 (if (<=
      (*
       (+ (pow (sin ky_m) 2.0) (pow (sin kx_m) 2.0))
       (pow (/ (* l 2.0) Om) 2.0))
      2.0)
   (sqrt (+ 0.5 0.5))
   (sqrt (* (+ (* -0.5 (/ Om (* (sin ky_m) l))) 1.0) (/ 1.0 2.0)))))

C

ky_m = fabs(ky);
kx_m = fabs(kx);
assert(l < Om && Om < kx_m && kx_m < ky_m);
double code(double l, double Om, double kx_m, double ky_m) {
	double tmp;
	if (((pow(sin(ky_m), 2.0) + pow(sin(kx_m), 2.0)) * pow(((l * 2.0) / Om), 2.0)) <= 2.0) {
		tmp = sqrt((0.5 + 0.5));
	} else {
		tmp = sqrt((((-0.5 * (Om / (sin(ky_m) * l))) + 1.0) * (1.0 / 2.0)));
	}
	return tmp;
}

Fortran

ky_m = abs(ky)
kx_m = abs(kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
real(8) function code(l, om, kx_m, ky_m)
    real(8), intent (in) :: l
    real(8), intent (in) :: om
    real(8), intent (in) :: kx_m
    real(8), intent (in) :: ky_m
    real(8) :: tmp
    if ((((sin(ky_m) ** 2.0d0) + (sin(kx_m) ** 2.0d0)) * (((l * 2.0d0) / om) ** 2.0d0)) <= 2.0d0) then
        tmp = sqrt((0.5d0 + 0.5d0))
    else
        tmp = sqrt(((((-0.5d0) * (om / (sin(ky_m) * l))) + 1.0d0) * (1.0d0 / 2.0d0)))
    end if
    code = tmp
end function

Java

ky_m = Math.abs(ky);
kx_m = Math.abs(kx);
assert l < Om && Om < kx_m && kx_m < ky_m;
public static double code(double l, double Om, double kx_m, double ky_m) {
	double tmp;
	if (((Math.pow(Math.sin(ky_m), 2.0) + Math.pow(Math.sin(kx_m), 2.0)) * Math.pow(((l * 2.0) / Om), 2.0)) <= 2.0) {
		tmp = Math.sqrt((0.5 + 0.5));
	} else {
		tmp = Math.sqrt((((-0.5 * (Om / (Math.sin(ky_m) * l))) + 1.0) * (1.0 / 2.0)));
	}
	return tmp;
}

Python

ky_m = math.fabs(ky)
kx_m = math.fabs(kx)
[l, Om, kx_m, ky_m] = sort([l, Om, kx_m, ky_m])
def code(l, Om, kx_m, ky_m):
	tmp = 0
	if ((math.pow(math.sin(ky_m), 2.0) + math.pow(math.sin(kx_m), 2.0)) * math.pow(((l * 2.0) / Om), 2.0)) <= 2.0:
		tmp = math.sqrt((0.5 + 0.5))
	else:
		tmp = math.sqrt((((-0.5 * (Om / (math.sin(ky_m) * l))) + 1.0) * (1.0 / 2.0)))
	return tmp

Julia

ky_m = abs(ky)
kx_m = abs(kx)
l, Om, kx_m, ky_m = sort([l, Om, kx_m, ky_m])
function code(l, Om, kx_m, ky_m)
	tmp = 0.0
	if (Float64(Float64((sin(ky_m) ^ 2.0) + (sin(kx_m) ^ 2.0)) * (Float64(Float64(l * 2.0) / Om) ^ 2.0)) <= 2.0)
		tmp = sqrt(Float64(0.5 + 0.5));
	else
		tmp = sqrt(Float64(Float64(Float64(-0.5 * Float64(Om / Float64(sin(ky_m) * l))) + 1.0) * Float64(1.0 / 2.0)));
	end
	return tmp
end

MATLAB

ky_m = abs(ky);
kx_m = abs(kx);
l, Om, kx_m, ky_m = num2cell(sort([l, Om, kx_m, ky_m])){:}
function tmp_2 = code(l, Om, kx_m, ky_m)
	tmp = 0.0;
	if ((((sin(ky_m) ^ 2.0) + (sin(kx_m) ^ 2.0)) * (((l * 2.0) / Om) ^ 2.0)) <= 2.0)
		tmp = sqrt((0.5 + 0.5));
	else
		tmp = sqrt((((-0.5 * (Om / (sin(ky_m) * l))) + 1.0) * (1.0 / 2.0)));
	end
	tmp_2 = tmp;
end

Wolfram

ky_m = N[Abs[ky], $MachinePrecision]
kx_m = N[Abs[kx], $MachinePrecision]
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
code[l_, Om_, kx$95$m_, ky$95$m_] := If[LessEqual[N[(N[(N[Power[N[Sin[ky$95$m], $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[Sin[kx$95$m], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] * N[Power[N[(N[(l * 2.0), $MachinePrecision] / Om), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision], 2.0], N[Sqrt[N[(0.5 + 0.5), $MachinePrecision]], $MachinePrecision], N[Sqrt[N[(N[(N[(-0.5 * N[(Om / N[(N[Sin[ky$95$m], $MachinePrecision] * l), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + 1.0), $MachinePrecision] * N[(1.0 / 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Derivation

1. Split input into 2 regimes

2. if (*.f64 (pow.f64 (/.f64 (*.f64 #s(literal 2 binary64) l) Om) #s(literal 2 binary64)) (+.f64 (pow.f64 (sin.f64 kx) #s(literal 2 binary64)) (pow.f64 (sin.f64 ky) #s(literal 2 binary64)))) < 2

   1. Initial program 100.0%

      \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
   2. Add Preprocessing

   3. Taylor expanded in l around 0

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
   4. Step-by-step derivation

   5. Applied rewrites 97.5%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
   6. Step-by-step derivation

      1. lift-*.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2} \cdot \left(1 + \frac{1}{1}\right)}} \]

      2. lift-/.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} \cdot \left(1 + \frac{1}{1}\right)} \]

      3. metadata-eval N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} \cdot \left(1 + \frac{1}{1}\right)} \]

      4. lift-+.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \color{blue}{\left(1 + \frac{1}{1}\right)}} \]

      5. +-commutative N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \color{blue}{\left(\frac{1}{1} + 1\right)}} \]

      6. distribute-rgt-in N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{1} \cdot \frac{1}{2} + 1 \cdot \frac{1}{2}}} \]

      7. metadata-eval N/A

         \[\leadsto \sqrt{\frac{1}{1} \cdot \frac{1}{2} + \color{blue}{\frac{1}{2}}} \]

      8. lower-+.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{1} \cdot \frac{1}{2} + \frac{1}{2}}} \]

   7. Applied rewrites 97.5%

      \[\leadsto \color{blue}{\sqrt{\frac{0.5}{1} + 0.5}} \]

   8. Taylor expanded in l around 0

      \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} + \frac{1}{2}} \]
   9. Step-by-step derivation

   10. Applied rewrites 97.5%

       \[\leadsto \sqrt{\color{blue}{0.5} + 0.5} \]

   if 2 < (*.f64 (pow.f64 (/.f64 (*.f64 #s(literal 2 binary64) l) Om) #s(literal 2 binary64)) (+.f64 (pow.f64 (sin.f64 kx) #s(literal 2 binary64)) (pow.f64 (sin.f64 ky) #s(literal 2 binary64))))

   1. Initial program 98.1%

      \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
   2. Add Preprocessing

   3. Taylor expanded in kx around 0

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]
   4. Step-by-step derivation

      1. lower-sqrt.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]

      2. lower-/.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\color{blue}{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]

      3. +-commutative N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}} + 1}}}\right)} \]

      4. associate-/l* N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{4 \cdot \color{blue}{\left({\ell}^{2} \cdot \frac{{\sin ky}^{2}}{{Om}^{2}}\right)} + 1}}\right)} \]

      5. associate-*r* N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{\left(4 \cdot {\ell}^{2}\right) \cdot \frac{{\sin ky}^{2}}{{Om}^{2}}} + 1}}\right)} \]

      6. lower-fma.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{\mathsf{fma}\left(4 \cdot {\ell}^{2}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}}\right)} \]

      7. lower-*.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(\color{blue}{4 \cdot {\ell}^{2}}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      8. unpow2 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \color{blue}{\left(\ell \cdot \ell\right)}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      9. lower-*.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \color{blue}{\left(\ell \cdot \ell\right)}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      10. lower-/.f64 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \color{blue}{\frac{{\sin ky}^{2}}{{Om}^{2}}}, 1\right)}}\right)} \]

      11. lower-pow.f64 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{\color{blue}{{\sin ky}^{2}}}{{Om}^{2}}, 1\right)}}\right)} \]

      12. lower-sin.f64 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\color{blue}{\sin ky}}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      13. unpow2 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{\color{blue}{Om \cdot Om}}, 1\right)}}\right)} \]

      14. lower-*.f64 70.1

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{\color{blue}{Om \cdot Om}}, 1\right)}}\right)} \]

   5. Applied rewrites 70.1%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{Om \cdot Om}, 1\right)}}}\right)} \]

   6. Taylor expanded in l around -inf

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{-1}{2} \cdot \color{blue}{\frac{Om}{\ell \cdot \sin ky}}\right)} \]
   7. Step-by-step derivation

   8. Applied rewrites 81.4%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{Om}{\sin ky \cdot \ell} \cdot \color{blue}{-0.5}\right)} \]
3. Recombined 2 regimes into one program.

4. Final simplification 90.8%

   \[\leadsto \begin{array}{l} \mathbf{if}\;\left({\sin ky}^{2} + {\sin kx}^{2}\right) \cdot {\left(\frac{\ell \cdot 2}{Om}\right)}^{2} \leq 2:\\ \;\;\;\;\sqrt{0.5 + 0.5}\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\left(-0.5 \cdot \frac{Om}{\sin ky \cdot \ell} + 1\right) \cdot \frac{1}{2}}\\ \end{array} \]
5. Add Preprocessing

Alternative 4: 98.3% accurate, 1.0× speedup

Math

\[\begin{array}{l} ky_m = \left|ky\right| \\ kx_m = \left|kx\right| \\ [l, Om, kx_m, ky_m] = \mathsf{sort}([l, Om, kx_m, ky_m])\\ \\ \begin{array}{l} \mathbf{if}\;\left({\sin ky\_m}^{2} + {\sin kx\_m}^{2}\right) \cdot {\left(\frac{\ell \cdot 2}{Om}\right)}^{2} \leq 0.4:\\ \;\;\;\;\sqrt{0.5 + 0.5}\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\left(\frac{Om}{ky\_m \cdot \ell} \cdot 0.5 + 1\right) \cdot \frac{1}{2}}\\ \end{array} \end{array} \]

FPCore

ky_m = (fabs.f64 ky)
kx_m = (fabs.f64 kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
(FPCore (l Om kx_m ky_m)
 :precision binary64
 (if (<=
      (*
       (+ (pow (sin ky_m) 2.0) (pow (sin kx_m) 2.0))
       (pow (/ (* l 2.0) Om) 2.0))
      0.4)
   (sqrt (+ 0.5 0.5))
   (sqrt (* (+ (* (/ Om (* ky_m l)) 0.5) 1.0) (/ 1.0 2.0)))))

C

ky_m = fabs(ky);
kx_m = fabs(kx);
assert(l < Om && Om < kx_m && kx_m < ky_m);
double code(double l, double Om, double kx_m, double ky_m) {
	double tmp;
	if (((pow(sin(ky_m), 2.0) + pow(sin(kx_m), 2.0)) * pow(((l * 2.0) / Om), 2.0)) <= 0.4) {
		tmp = sqrt((0.5 + 0.5));
	} else {
		tmp = sqrt(((((Om / (ky_m * l)) * 0.5) + 1.0) * (1.0 / 2.0)));
	}
	return tmp;
}

Fortran

ky_m = abs(ky)
kx_m = abs(kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
real(8) function code(l, om, kx_m, ky_m)
    real(8), intent (in) :: l
    real(8), intent (in) :: om
    real(8), intent (in) :: kx_m
    real(8), intent (in) :: ky_m
    real(8) :: tmp
    if ((((sin(ky_m) ** 2.0d0) + (sin(kx_m) ** 2.0d0)) * (((l * 2.0d0) / om) ** 2.0d0)) <= 0.4d0) then
        tmp = sqrt((0.5d0 + 0.5d0))
    else
        tmp = sqrt(((((om / (ky_m * l)) * 0.5d0) + 1.0d0) * (1.0d0 / 2.0d0)))
    end if
    code = tmp
end function

Java

ky_m = Math.abs(ky);
kx_m = Math.abs(kx);
assert l < Om && Om < kx_m && kx_m < ky_m;
public static double code(double l, double Om, double kx_m, double ky_m) {
	double tmp;
	if (((Math.pow(Math.sin(ky_m), 2.0) + Math.pow(Math.sin(kx_m), 2.0)) * Math.pow(((l * 2.0) / Om), 2.0)) <= 0.4) {
		tmp = Math.sqrt((0.5 + 0.5));
	} else {
		tmp = Math.sqrt(((((Om / (ky_m * l)) * 0.5) + 1.0) * (1.0 / 2.0)));
	}
	return tmp;
}

Python

ky_m = math.fabs(ky)
kx_m = math.fabs(kx)
[l, Om, kx_m, ky_m] = sort([l, Om, kx_m, ky_m])
def code(l, Om, kx_m, ky_m):
	tmp = 0
	if ((math.pow(math.sin(ky_m), 2.0) + math.pow(math.sin(kx_m), 2.0)) * math.pow(((l * 2.0) / Om), 2.0)) <= 0.4:
		tmp = math.sqrt((0.5 + 0.5))
	else:
		tmp = math.sqrt(((((Om / (ky_m * l)) * 0.5) + 1.0) * (1.0 / 2.0)))
	return tmp

Julia

ky_m = abs(ky)
kx_m = abs(kx)
l, Om, kx_m, ky_m = sort([l, Om, kx_m, ky_m])
function code(l, Om, kx_m, ky_m)
	tmp = 0.0
	if (Float64(Float64((sin(ky_m) ^ 2.0) + (sin(kx_m) ^ 2.0)) * (Float64(Float64(l * 2.0) / Om) ^ 2.0)) <= 0.4)
		tmp = sqrt(Float64(0.5 + 0.5));
	else
		tmp = sqrt(Float64(Float64(Float64(Float64(Om / Float64(ky_m * l)) * 0.5) + 1.0) * Float64(1.0 / 2.0)));
	end
	return tmp
end

MATLAB

ky_m = abs(ky);
kx_m = abs(kx);
l, Om, kx_m, ky_m = num2cell(sort([l, Om, kx_m, ky_m])){:}
function tmp_2 = code(l, Om, kx_m, ky_m)
	tmp = 0.0;
	if ((((sin(ky_m) ^ 2.0) + (sin(kx_m) ^ 2.0)) * (((l * 2.0) / Om) ^ 2.0)) <= 0.4)
		tmp = sqrt((0.5 + 0.5));
	else
		tmp = sqrt(((((Om / (ky_m * l)) * 0.5) + 1.0) * (1.0 / 2.0)));
	end
	tmp_2 = tmp;
end

Wolfram

ky_m = N[Abs[ky], $MachinePrecision]
kx_m = N[Abs[kx], $MachinePrecision]
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
code[l_, Om_, kx$95$m_, ky$95$m_] := If[LessEqual[N[(N[(N[Power[N[Sin[ky$95$m], $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[Sin[kx$95$m], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] * N[Power[N[(N[(l * 2.0), $MachinePrecision] / Om), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision], 0.4], N[Sqrt[N[(0.5 + 0.5), $MachinePrecision]], $MachinePrecision], N[Sqrt[N[(N[(N[(N[(Om / N[(ky$95$m * l), $MachinePrecision]), $MachinePrecision] * 0.5), $MachinePrecision] + 1.0), $MachinePrecision] * N[(1.0 / 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]

Derivation

1. Split input into 2 regimes

2. if (*.f64 (pow.f64 (/.f64 (*.f64 #s(literal 2 binary64) l) Om) #s(literal 2 binary64)) (+.f64 (pow.f64 (sin.f64 kx) #s(literal 2 binary64)) (pow.f64 (sin.f64 ky) #s(literal 2 binary64)))) < 0.40000000000000002

   1. Initial program 100.0%

      \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
   2. Add Preprocessing

   3. Taylor expanded in l around 0

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
   4. Step-by-step derivation

   5. Applied rewrites 98.0%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
   6. Step-by-step derivation

      1. lift-*.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2} \cdot \left(1 + \frac{1}{1}\right)}} \]

      2. lift-/.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} \cdot \left(1 + \frac{1}{1}\right)} \]

      3. metadata-eval N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} \cdot \left(1 + \frac{1}{1}\right)} \]

      4. lift-+.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \color{blue}{\left(1 + \frac{1}{1}\right)}} \]

      5. +-commutative N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \color{blue}{\left(\frac{1}{1} + 1\right)}} \]

      6. distribute-rgt-in N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{1} \cdot \frac{1}{2} + 1 \cdot \frac{1}{2}}} \]

      7. metadata-eval N/A

         \[\leadsto \sqrt{\frac{1}{1} \cdot \frac{1}{2} + \color{blue}{\frac{1}{2}}} \]

      8. lower-+.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{1} \cdot \frac{1}{2} + \frac{1}{2}}} \]

   7. Applied rewrites 98.0%

      \[\leadsto \color{blue}{\sqrt{\frac{0.5}{1} + 0.5}} \]

   8. Taylor expanded in l around 0

      \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} + \frac{1}{2}} \]
   9. Step-by-step derivation

   10. Applied rewrites 98.0%

       \[\leadsto \sqrt{\color{blue}{0.5} + 0.5} \]

   if 0.40000000000000002 < (*.f64 (pow.f64 (/.f64 (*.f64 #s(literal 2 binary64) l) Om) #s(literal 2 binary64)) (+.f64 (pow.f64 (sin.f64 kx) #s(literal 2 binary64)) (pow.f64 (sin.f64 ky) #s(literal 2 binary64))))

   1. Initial program 98.1%

      \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
   2. Add Preprocessing

   3. Taylor expanded in kx around 0

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]
   4. Step-by-step derivation

      1. lower-sqrt.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]

      2. lower-/.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\color{blue}{\frac{1}{1 + 4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}}}}}\right)} \]

      3. +-commutative N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{4 \cdot \frac{{\ell}^{2} \cdot {\sin ky}^{2}}{{Om}^{2}} + 1}}}\right)} \]

      4. associate-/l* N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{4 \cdot \color{blue}{\left({\ell}^{2} \cdot \frac{{\sin ky}^{2}}{{Om}^{2}}\right)} + 1}}\right)} \]

      5. associate-*r* N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{\left(4 \cdot {\ell}^{2}\right) \cdot \frac{{\sin ky}^{2}}{{Om}^{2}}} + 1}}\right)} \]

      6. lower-fma.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\color{blue}{\mathsf{fma}\left(4 \cdot {\ell}^{2}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}}\right)} \]

      7. lower-*.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(\color{blue}{4 \cdot {\ell}^{2}}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      8. unpow2 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \color{blue}{\left(\ell \cdot \ell\right)}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      9. lower-*.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \color{blue}{\left(\ell \cdot \ell\right)}, \frac{{\sin ky}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      10. lower-/.f64 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \color{blue}{\frac{{\sin ky}^{2}}{{Om}^{2}}}, 1\right)}}\right)} \]

      11. lower-pow.f64 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{\color{blue}{{\sin ky}^{2}}}{{Om}^{2}}, 1\right)}}\right)} \]

      12. lower-sin.f64 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\color{blue}{\sin ky}}^{2}}{{Om}^{2}}, 1\right)}}\right)} \]

      13. unpow2 N/A

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{\color{blue}{Om \cdot Om}}, 1\right)}}\right)} \]

      14. lower-*.f64 69.7

          \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{\color{blue}{Om \cdot Om}}, 1\right)}}\right)} \]

   5. Applied rewrites 69.7%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \color{blue}{\sqrt{\frac{1}{\mathsf{fma}\left(4 \cdot \left(\ell \cdot \ell\right), \frac{{\sin ky}^{2}}{Om \cdot Om}, 1\right)}}}\right)} \]

   6. Taylor expanded in l around inf

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{2} \cdot \color{blue}{\frac{Om}{\ell \cdot \sin ky}}\right)} \]
   7. Step-by-step derivation

   8. Applied rewrites 80.6%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{Om}{\sin ky \cdot \ell} \cdot \color{blue}{0.5}\right)} \]

   9. Taylor expanded in ky around 0

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{Om}{ky \cdot \ell} \cdot \frac{1}{2}\right)} \]
   10. Step-by-step derivation

   11. Applied rewrites 80.1%

       \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{Om}{\ell \cdot ky} \cdot 0.5\right)} \]
3. Recombined 2 regimes into one program.

4. Final simplification 90.5%

   \[\leadsto \begin{array}{l} \mathbf{if}\;\left({\sin ky}^{2} + {\sin kx}^{2}\right) \cdot {\left(\frac{\ell \cdot 2}{Om}\right)}^{2} \leq 0.4:\\ \;\;\;\;\sqrt{0.5 + 0.5}\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\left(\frac{Om}{ky \cdot \ell} \cdot 0.5 + 1\right) \cdot \frac{1}{2}}\\ \end{array} \]
5. Add Preprocessing

Alternative 5: 98.2% accurate, 1.1× speedup

Math

\[\begin{array}{l} ky_m = \left|ky\right| \\ kx_m = \left|kx\right| \\ [l, Om, kx_m, ky_m] = \mathsf{sort}([l, Om, kx_m, ky_m])\\ \\ \begin{array}{l} \mathbf{if}\;\left({\sin ky\_m}^{2} + {\sin kx\_m}^{2}\right) \cdot {\left(\frac{\ell \cdot 2}{Om}\right)}^{2} \leq 3.8:\\ \;\;\;\;\sqrt{0.5 + 0.5}\\ \mathbf{else}:\\ \;\;\;\;\sqrt{0.5}\\ \end{array} \end{array} \]

FPCore

ky_m = (fabs.f64 ky)
kx_m = (fabs.f64 kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
(FPCore (l Om kx_m ky_m)
 :precision binary64
 (if (<=
      (*
       (+ (pow (sin ky_m) 2.0) (pow (sin kx_m) 2.0))
       (pow (/ (* l 2.0) Om) 2.0))
      3.8)
   (sqrt (+ 0.5 0.5))
   (sqrt 0.5)))

C

ky_m = fabs(ky);
kx_m = fabs(kx);
assert(l < Om && Om < kx_m && kx_m < ky_m);
double code(double l, double Om, double kx_m, double ky_m) {
	double tmp;
	if (((pow(sin(ky_m), 2.0) + pow(sin(kx_m), 2.0)) * pow(((l * 2.0) / Om), 2.0)) <= 3.8) {
		tmp = sqrt((0.5 + 0.5));
	} else {
		tmp = sqrt(0.5);
	}
	return tmp;
}

Fortran

ky_m = abs(ky)
kx_m = abs(kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
real(8) function code(l, om, kx_m, ky_m)
    real(8), intent (in) :: l
    real(8), intent (in) :: om
    real(8), intent (in) :: kx_m
    real(8), intent (in) :: ky_m
    real(8) :: tmp
    if ((((sin(ky_m) ** 2.0d0) + (sin(kx_m) ** 2.0d0)) * (((l * 2.0d0) / om) ** 2.0d0)) <= 3.8d0) then
        tmp = sqrt((0.5d0 + 0.5d0))
    else
        tmp = sqrt(0.5d0)
    end if
    code = tmp
end function

Java

ky_m = Math.abs(ky);
kx_m = Math.abs(kx);
assert l < Om && Om < kx_m && kx_m < ky_m;
public static double code(double l, double Om, double kx_m, double ky_m) {
	double tmp;
	if (((Math.pow(Math.sin(ky_m), 2.0) + Math.pow(Math.sin(kx_m), 2.0)) * Math.pow(((l * 2.0) / Om), 2.0)) <= 3.8) {
		tmp = Math.sqrt((0.5 + 0.5));
	} else {
		tmp = Math.sqrt(0.5);
	}
	return tmp;
}

Python

ky_m = math.fabs(ky)
kx_m = math.fabs(kx)
[l, Om, kx_m, ky_m] = sort([l, Om, kx_m, ky_m])
def code(l, Om, kx_m, ky_m):
	tmp = 0
	if ((math.pow(math.sin(ky_m), 2.0) + math.pow(math.sin(kx_m), 2.0)) * math.pow(((l * 2.0) / Om), 2.0)) <= 3.8:
		tmp = math.sqrt((0.5 + 0.5))
	else:
		tmp = math.sqrt(0.5)
	return tmp

Julia

ky_m = abs(ky)
kx_m = abs(kx)
l, Om, kx_m, ky_m = sort([l, Om, kx_m, ky_m])
function code(l, Om, kx_m, ky_m)
	tmp = 0.0
	if (Float64(Float64((sin(ky_m) ^ 2.0) + (sin(kx_m) ^ 2.0)) * (Float64(Float64(l * 2.0) / Om) ^ 2.0)) <= 3.8)
		tmp = sqrt(Float64(0.5 + 0.5));
	else
		tmp = sqrt(0.5);
	end
	return tmp
end

MATLAB

ky_m = abs(ky);
kx_m = abs(kx);
l, Om, kx_m, ky_m = num2cell(sort([l, Om, kx_m, ky_m])){:}
function tmp_2 = code(l, Om, kx_m, ky_m)
	tmp = 0.0;
	if ((((sin(ky_m) ^ 2.0) + (sin(kx_m) ^ 2.0)) * (((l * 2.0) / Om) ^ 2.0)) <= 3.8)
		tmp = sqrt((0.5 + 0.5));
	else
		tmp = sqrt(0.5);
	end
	tmp_2 = tmp;
end

Wolfram

ky_m = N[Abs[ky], $MachinePrecision]
kx_m = N[Abs[kx], $MachinePrecision]
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
code[l_, Om_, kx$95$m_, ky$95$m_] := If[LessEqual[N[(N[(N[Power[N[Sin[ky$95$m], $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[Sin[kx$95$m], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] * N[Power[N[(N[(l * 2.0), $MachinePrecision] / Om), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision], 3.8], N[Sqrt[N[(0.5 + 0.5), $MachinePrecision]], $MachinePrecision], N[Sqrt[0.5], $MachinePrecision]]

Derivation

1. Split input into 2 regimes

2. if (*.f64 (pow.f64 (/.f64 (*.f64 #s(literal 2 binary64) l) Om) #s(literal 2 binary64)) (+.f64 (pow.f64 (sin.f64 kx) #s(literal 2 binary64)) (pow.f64 (sin.f64 ky) #s(literal 2 binary64)))) < 3.7999999999999998

   1. Initial program 100.0%

      \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
   2. Add Preprocessing

   3. Taylor expanded in l around 0

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
   4. Step-by-step derivation

   5. Applied rewrites 97.5%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
   6. Step-by-step derivation

      1. lift-*.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2} \cdot \left(1 + \frac{1}{1}\right)}} \]

      2. lift-/.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} \cdot \left(1 + \frac{1}{1}\right)} \]

      3. metadata-eval N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} \cdot \left(1 + \frac{1}{1}\right)} \]

      4. lift-+.f64 N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \color{blue}{\left(1 + \frac{1}{1}\right)}} \]

      5. +-commutative N/A

         \[\leadsto \sqrt{\frac{1}{2} \cdot \color{blue}{\left(\frac{1}{1} + 1\right)}} \]

      6. distribute-rgt-in N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{1} \cdot \frac{1}{2} + 1 \cdot \frac{1}{2}}} \]

      7. metadata-eval N/A

         \[\leadsto \sqrt{\frac{1}{1} \cdot \frac{1}{2} + \color{blue}{\frac{1}{2}}} \]

      8. lower-+.f64 N/A

         \[\leadsto \sqrt{\color{blue}{\frac{1}{1} \cdot \frac{1}{2} + \frac{1}{2}}} \]

   7. Applied rewrites 97.5%

      \[\leadsto \color{blue}{\sqrt{\frac{0.5}{1} + 0.5}} \]

   8. Taylor expanded in l around 0

      \[\leadsto \sqrt{\color{blue}{\frac{1}{2}} + \frac{1}{2}} \]
   9. Step-by-step derivation

   10. Applied rewrites 97.5%

       \[\leadsto \sqrt{\color{blue}{0.5} + 0.5} \]

   if 3.7999999999999998 < (*.f64 (pow.f64 (/.f64 (*.f64 #s(literal 2 binary64) l) Om) #s(literal 2 binary64)) (+.f64 (pow.f64 (sin.f64 kx) #s(literal 2 binary64)) (pow.f64 (sin.f64 ky) #s(literal 2 binary64))))

   1. Initial program 98.1%

      \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
   2. Add Preprocessing

   3. Taylor expanded in l around 0

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
   4. Step-by-step derivation

   5. Applied rewrites 20.0%

      \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]

   6. Taylor expanded in l around inf

      \[\leadsto \color{blue}{\sqrt{\frac{1}{2}}} \]
   7. Step-by-step derivation

      1. lower-sqrt.f64 97.1

         \[\leadsto \color{blue}{\sqrt{0.5}} \]

   8. Applied rewrites 97.1%

      \[\leadsto \color{blue}{\sqrt{0.5}} \]
3. Recombined 2 regimes into one program.

4. Final simplification 97.4%

   \[\leadsto \begin{array}{l} \mathbf{if}\;\left({\sin ky}^{2} + {\sin kx}^{2}\right) \cdot {\left(\frac{\ell \cdot 2}{Om}\right)}^{2} \leq 3.8:\\ \;\;\;\;\sqrt{0.5 + 0.5}\\ \mathbf{else}:\\ \;\;\;\;\sqrt{0.5}\\ \end{array} \]
5. Add Preprocessing

Alternative 6: 55.9% accurate, 52.8× speedup

Math

\[\begin{array}{l} ky_m = \left|ky\right| \\ kx_m = \left|kx\right| \\ [l, Om, kx_m, ky_m] = \mathsf{sort}([l, Om, kx_m, ky_m])\\ \\ \sqrt{0.5} \end{array} \]

FPCore

ky_m = (fabs.f64 ky)
kx_m = (fabs.f64 kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
(FPCore (l Om kx_m ky_m) :precision binary64 (sqrt 0.5))

C

ky_m = fabs(ky);
kx_m = fabs(kx);
assert(l < Om && Om < kx_m && kx_m < ky_m);
double code(double l, double Om, double kx_m, double ky_m) {
	return sqrt(0.5);
}

Fortran

ky_m = abs(ky)
kx_m = abs(kx)
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
real(8) function code(l, om, kx_m, ky_m)
    real(8), intent (in) :: l
    real(8), intent (in) :: om
    real(8), intent (in) :: kx_m
    real(8), intent (in) :: ky_m
    code = sqrt(0.5d0)
end function

Java

ky_m = Math.abs(ky);
kx_m = Math.abs(kx);
assert l < Om && Om < kx_m && kx_m < ky_m;
public static double code(double l, double Om, double kx_m, double ky_m) {
	return Math.sqrt(0.5);
}

Python

ky_m = math.fabs(ky)
kx_m = math.fabs(kx)
[l, Om, kx_m, ky_m] = sort([l, Om, kx_m, ky_m])
def code(l, Om, kx_m, ky_m):
	return math.sqrt(0.5)

Julia

ky_m = abs(ky)
kx_m = abs(kx)
l, Om, kx_m, ky_m = sort([l, Om, kx_m, ky_m])
function code(l, Om, kx_m, ky_m)
	return sqrt(0.5)
end

MATLAB

ky_m = abs(ky);
kx_m = abs(kx);
l, Om, kx_m, ky_m = num2cell(sort([l, Om, kx_m, ky_m])){:}
function tmp = code(l, Om, kx_m, ky_m)
	tmp = sqrt(0.5);
end

Wolfram

ky_m = N[Abs[ky], $MachinePrecision]
kx_m = N[Abs[kx], $MachinePrecision]
NOTE: l, Om, kx_m, and ky_m should be sorted in increasing order before calling this function.
code[l_, Om_, kx$95$m_, ky$95$m_] := N[Sqrt[0.5], $MachinePrecision]

Derivation

1. Initial program 99.2%

   \[\sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\sqrt{1 + {\left(\frac{2 \cdot \ell}{Om}\right)}^{2} \cdot \left({\sin kx}^{2} + {\sin ky}^{2}\right)}}\right)} \]
2. Add Preprocessing

3. Taylor expanded in l around 0

   \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]
4. Step-by-step derivation

5. Applied rewrites 65.1%

   \[\leadsto \sqrt{\frac{1}{2} \cdot \left(1 + \frac{1}{\color{blue}{1}}\right)} \]

6. Taylor expanded in l around inf

   \[\leadsto \color{blue}{\sqrt{\frac{1}{2}}} \]
7. Step-by-step derivation

   1. lower-sqrt.f64 52.2

      \[\leadsto \color{blue}{\sqrt{0.5}} \]

8. Applied rewrites 52.2%

   \[\leadsto \color{blue}{\sqrt{0.5}} \]
9. Add Preprocessing

Reproduce

herbie shell --seed 2024312 
(FPCore (l Om kx ky)
  :name "Toniolo and Linder, Equation (3a)"
  :precision binary64
  (sqrt (* (/ 1.0 2.0) (+ 1.0 (/ 1.0 (sqrt (+ 1.0 (* (pow (/ (* 2.0 l) Om) 2.0) (+ (pow (sin kx) 2.0) (pow (sin ky) 2.0))))))))))