I'm having trouble with the slow computation of my Python code. Based on the pycallgraph below, the bottleneck seems to be the module named miepython.miepython.mie_S1_S2 (highlighted by pink), which takes 0.47 seconds per call.

The source code for this module is as follows:
import numpy as np
from numba import njit, int32, float64, complex128
__all__ = ('ez_mie',
'ez_intensities',
'generate_mie_costheta',
'i_par',
'i_per',
'i_unpolarized',
'mie',
'mie_S1_S2',
'mie_cdf',
'mie_mu_with_uniform_cdf',
)
@njit((complex128, float64, float64[:]), cache=True)
def _mie_S1_S2(m, x, mu):
"""
Calculate the scattering amplitude functions for spheres.
The amplitude functions have been normalized so that when integrated
over all 4*pi solid angles, the integral will be qext*pi*x**2.
The units are weird, sr**(-0.5)
Args:
m: the complex index of refraction of the sphere
x: the size parameter of the sphere
mu: array of angles, cos(theta), to calculate scattering amplitudes
Returns:
S1, S2: the scattering amplitudes at each angle mu [sr**(-0.5)]
"""
nstop = int(x + 4.05 * x**0.33333 + 2.0) + 1
a = np.zeros(nstop - 1, dtype=np.complex128)
b = np.zeros(nstop - 1, dtype=np.complex128)
_mie_An_Bn(m, x, a, b)
nangles = len(mu)
S1 = np.zeros(nangles, dtype=np.complex128)
S2 = np.zeros(nangles, dtype=np.complex128)
nstop = len(a)
for k in range(nangles):
pi_nm2 = 0
pi_nm1 = 1
for n in range(1, nstop):
tau_nm1 = n * mu[k] * pi_nm1 - (n + 1) * pi_nm2
S1[k] += (2 * n + 1) * (pi_nm1 * a[n - 1]
+ tau_nm1 * b[n - 1]) / (n + 1) / n
S2[k] += (2 * n + 1) * (tau_nm1 * a[n - 1]
+ pi_nm1 * b[n - 1]) / (n + 1) / n
temp = pi_nm1
pi_nm1 = ((2 * n + 1) * mu[k] * pi_nm1 - (n + 1) * pi_nm2) / n
pi_nm2 = temp
# calculate norm = sqrt(pi * Qext * x**2)
n = np.arange(1, nstop + 1)
norm = np.sqrt(2 * np.pi * np.sum((2 * n + 1) * (a.real + b.real)))
S1 /= norm
S2 /= norm
return [S1, S2]
Apparently, the source code is jitted by Numba so it should be faster than it actually is. The number of iterations in for loop in this function is around 25,000 (len(mu)=50, len(a)-1=500).
Any ideas on how to speed up this computation? Is something hindering the fast computation of Numba? Or, do you think the computation is already fast enough?
[More details]
In the above, another function _mie_An_Bn is being used. This function is also jitted, and the source code is as follows:
@njit((complex128, float64, complex128[:], complex128[:]), cache=True)
def _mie_An_Bn(m, x, a, b):
"""
Compute arrays of Mie coefficients A and B for a sphere.
This estimates the size of the arrays based on Wiscombe's formula. The length
of the arrays is chosen so that the error when the series are summed is
around 1e-6.
Args:
m: the complex index of refraction of the sphere
x: the size parameter of the sphere
Returns:
An, Bn: arrays of Mie coefficents
"""
psi_nm1 = np.sin(x) # nm1 = n-1 = 0
psi_n = psi_nm1 / x - np.cos(x) # n = 1
xi_nm1 = complex(psi_nm1, np.cos(x))
xi_n = complex(psi_n, np.cos(x) / x + np.sin(x))
nstop = len(a)
if m.real > 0.0:
D = _D_calc(m, x, nstop + 1)
for n in range(1, nstop):
temp = D[n] / m + n / x
a[n - 1] = (temp * psi_n - psi_nm1) / (temp * xi_n - xi_nm1)
temp = D[n] * m + n / x
b[n - 1] = (temp * psi_n - psi_nm1) / (temp * xi_n - xi_nm1)
xi = (2 * n + 1) * xi_n / x - xi_nm1
xi_nm1 = xi_n
xi_n = xi
psi_nm1 = psi_n
psi_n = xi_n.real
else:
for n in range(1, nstop):
a[n - 1] = (n * psi_n / x - psi_nm1) / (n * xi_n / x - xi_nm1)
b[n - 1] = psi_n / xi_n
xi = (2 * n + 1) * xi_n / x - xi_nm1
xi_nm1 = xi_n
xi_n = xi
psi_nm1 = psi_n
psi_n = xi_n.real
The example inputs are like the followings:
m = 1.336-2.462e-09j
x = 8526.95
mu = np.array([-1., -0.7500396, 0.46037385, 0.5988121, 0.67384093, 0.72468684, 0.76421644, 0.79175856, 0.81723714, 0.83962897, 0.85924182, 0.87641596, 0.89383665, 0.90708978, 0.91931481, 0.93067567, 0.94073113, 0.94961222, 0.95689496, 0.96467123, 0.97138347, 0.97791831, 0.98339434, 0.98870543, 0.99414948, 0.9975728 0.9989995, 0.9989995, 0.9989995, 0.9989995, 0.9989995,0.99899951, 0.99899951, 0.99899951, 0.99899951, 0.99899951, 0.99899951, 0.99899951, 0.99899951, 0.99899951, 0.99899952, 0.99899952,
0.99899952, 0.99899952, 0.99899952, 0.99899952, 0.99899952, 0.99899952, 0.99899952, 1. ])