scatt/examples/Opt.Commun.-2010-Geints-Nanojets_of_dielectric_microspheres/fig1.py

#!/usr/bin/env python3
# -*- coding: UTF-8 -*-
#
#    Copyright (C) 2009-2015 Ovidio Peña Rodríguez <ovidio@bytesfall.com>
#    Copyright (C) 2013-2015  Konstantin Ladutenko <kostyfisik@gmail.com>
#
#    This file is part of python-scattnlay
#
#    This program is free software: you can redistribute it and/or modify
#    it under the terms of the GNU General Public License as published by
#    the Free Software Foundation, either version 3 of the License, or
#    (at your option) any later version.
#
#    This program is distributed in the hope that it will be useful,
#    but WITHOUT ANY WARRANTY; without even the implied warranty of
#    MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
#    GNU General Public License for more details.
#
#    The only additional remark is that we expect that all publications
#    describing work using this software, or all commercial products
#    using it, cite at least one of the following references:
#    [1] O. Pena and U. Pal, "Scattering of electromagnetic radiation by
#        a multilayered sphere," Computer Physics Communications,
#        vol. 180, Nov. 2009, pp. 2348-2354.
#    [2] K. Ladutenko, U. Pal, A. Rivera, and O. Pena-Rodriguez, "Mie
#        calculation of electromagnetic near-field for a multilayered
#        sphere," Computer Physics Communications, vol. 214, May 2017,
#        pp. 225-230.
#
#    You should have received a copy of the GNU General Public License
#    along with this program.  If not, see <http:#www.gnu.org/licenses/>.

import scattnlay
from scattnlay import fieldnlay, scattnlay
import numpy as np
from matplotlib import pyplot as plt

import inspect

print("Using scattnlay from ", inspect.getfile(scattnlay))

npts = 11
# npts = 11
factor = 2  # plot extent compared to sphere radius
index_H2O = 1.33 + (1e-6) * 1j

WL = 0.532  # mkm
total_r = 125  # mkm
# isMP = False
isMP = True


nm = 1.0  # host medium
# x = 2.0 * np.pi * np.array([total_r/2, total_r], dtype=np.float64) / WL
# m = np.array((index_H2O, index_H2O), dtype=np.complex128) / nm

x = 2.0 * np.pi * np.array([total_r], dtype=np.float64) / WL
m = np.array((index_H2O), dtype=np.complex128) / nm

nmax = int(np.max(x * factor + 11 * (x * factor) ** (1.0 / 3.0) + 1))
# return std::round(x + 11 * std::pow(x, (1.0 / 3.0)) + 1);

# nmax = -1

print("x =", x)
print("m =", m)
terms, Qext, Qsca, Qabs, Qbk, Qpr, g, Albedo, S1, S2 = scattnlay(
    np.array([x]), np.array([m])
)
print("   Qsca = " + str(Qsca) + " terms = " + str(terms))
terms, Qext, Qsca, Qabs, Qbk, Qpr, g, Albedo, S1, S2 = scattnlay(
    np.array([x]), np.array([m]), mp=True
)
print("mp Qsca = " + str(Qsca) + " terms = " + str(terms))

scan = np.linspace(-factor * x[-1], factor * x[-1], npts)
zero = np.zeros(npts * npts, dtype=np.float64)

coordX, coordZ = np.meshgrid(scan, scan)
coordX.resize(npts * npts)
coordZ.resize(npts * npts)
coordY = zero

terms, E, H = fieldnlay(
    np.array([x]), np.array([m]), coordX, coordY, coordZ, mp=isMP, nmax=nmax
)
Ec = E[0, :, :]
Er = np.absolute(Ec)
Eabs2 = Er[:, 0] ** 2 + Er[:, 1] ** 2 + Er[:, 2] ** 2
Eabs_data = np.resize(Eabs2, (npts, npts))
label = r"$|E|^2$"
pos = plt.imshow(
    Eabs_data.T,
    cmap="gnuplot",
    # cmap='jet',
    vmin=0.0,
    vmax=14,
)
plt.colorbar(pos)
print(
    np.min(Eabs_data),
    np.max(Eabs_data),
    " terms = " + str(terms),
    " size=",
    Eabs_data.size,
)
mp = ""
if isMP:
    mp = "_mp"
plt.savefig("R" + str(total_r) + "mkm" + mp + ".jpg", dpi=300)
# plt.show()