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35 changes: 27 additions & 8 deletions bdsf/functions.py
Original file line number Diff line number Diff line change
Expand Up @@ -200,18 +200,37 @@ def gdist_pa(pix1, pix2, gsize):
return fwhm

def gaus_2d(c, x, y):
""" x and y are 2d arrays with the x and y positions. """
""" x and y are 2d arrays with the x and y positions.
c = [amp, x0, y0, sigx, sigy, pa_deg] """
import math
import numpy as N

# Pre-calculate rotation parameters outside of matrix operations
rad = 180.0/math.pi
cs = math.cos(c[5]/rad)
sn = math.sin(c[5]/rad)
f1 = ((x-c[1])*cs+(y-c[2])*sn)/c[3]
f2 = ((y-c[2])*cs-(x-c[1])*sn)/c[4]
val = c[0]*N.exp(-0.5*(f1*f1+f2*f2))

return val
angle_rad = c[5]/rad
cs = math.cos(angle_rad)
sn = math.sin(angle_rad)

# Coordinate shift
dx = x - c[1]
dy = y - c[2]
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# Avoiding the creation of unnecessary temporary arrays. The original function divided
# values before squaring, which created additional matrix copies in memory. The new
# version multiplies by the inverse of the square, which is a more computationally
# efficient.
inv_sigx2 = -0.5 / (c[3]**2)
inv_sigy2 = -0.5 / (c[4]**2)

# (f1^2 + f2^2) can be expressed as a quadratic form, which is computed faster by NumPy
# f1 = (dx*cs + dy*sn) / sigx
# f2 = (dy*cs - dx*sn) / sigy
f1_part = dx * cs + dy * sn
f2_part = dy * cs - dx * sn

exponent = (f1_part**2 * inv_sigx2) + (f2_part**2 * inv_sigy2)

return c[0] * N.exp(exponent)

def gaus_2d_itscomplicated(c, x, y, p_tofix, ind):
""" x and y are 2d arrays with the x and y positions. c is a list (of lists) of gaussian parameters to fit, p_tofix
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