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+#!/usr/bin/env python
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+# -*- coding: UTF-8 -*-
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+#
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+# Copyright (C) 2009-2015 Ovidio Peña Rodríguez <ovidio@bytesfall.com>
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+#
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+# This file is part of python-scattnlay
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+#
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+# This program is free software: you can redistribute it and/or modify
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+# it under the terms of the GNU General Public License as published by
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+# the Free Software Foundation, either version 3 of the License, or
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+# (at your option) any later version.
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+#
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+# This program is distributed in the hope that it will be useful,
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+# but WITHOUT ANY WARRANTY; without even the implied warranty of
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+# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
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+# GNU General Public License for more details.
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+#
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+# The only additional remark is that we expect that all publications
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+# describing work using this software, or all commercial products
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+# using it, cite the following reference:
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+# [1] O. Pena and U. Pal, "Scattering of electromagnetic radiation by
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+# a multilayered sphere," Computer Physics Communications,
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+# vol. 180, Nov. 2009, pp. 2348-2354.
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+#
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+# You should have received a copy of the GNU General Public License
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+# along with this program. If not, see <http://www.gnu.org/licenses/>.
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+
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+# This test case calculates the electric field in the
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+# E-k plane, for an spherical Si-Ag-Si nanoparticle. Core radius is 17.74 nm,
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+# inner layer 23.31nm, outer layer 22.95nm. Working wavelength is 800nm, we use
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+# silicon epsilon=13.64+i0.047, silver epsilon= -28.05+i1.525
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+
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+import os, cmath
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+import numpy as np
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+from scattnlay import fieldnlay
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+from fieldplot import fieldplot
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+
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+
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+if __name__ == '__main__':
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+ import argparse
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+
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+ parser = argparse.ArgumentParser()
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+
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+ parser.add_argument("dirnames", nargs='*', default='.', help="read all data from DIR(S)")
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+ parser.add_argument("-f", "--filename", dest="fname", nargs='?', default=None,
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+ help="name of 'n' file")
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+ parser.add_argument("-w", "--wavelength", dest="wl", default=3.75, type=float,
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+ help="wavelength of electromagnetic wave")
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+ parser.add_argument("-r", "--radius", dest="rad", default=None, type=float,
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+ help="radius of PEC sphere")
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+ parser.add_argument("-t", "--thickness", dest="tc", default=0.8, type=float,
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+ help="thickness of cloaking layer")
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+ parser.add_argument("-n", "--npoints", dest="npts", default=101, type=int,
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+ help="number of points for the grid")
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+
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+ args = parser.parse_args()
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+
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+ for dirname in args.dirnames:
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+ print "Calculating spectra for data file(s) in dir '%s'..." % (dirname)
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+
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+ wl = args.wl # cm
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+ if (args.rad is None):
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+ Rs = 0.75*wl # cm
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+ else:
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+ Rs = args.rad # cm
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+ tc = args.tc # cm
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+
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+ if (args.fname is None):
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+ files = [x for x in os.listdir('%s/' % (dirname)) if x.endswith('.dat')]
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+ files.sort()
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+ else:
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+ files = [args.fname]
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+
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+ npts = args.npts # cm
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+
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+ if not os.path.exists('%s/flow-results/' % (dirname)):
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+ os.makedirs('%s/flow-results/' % (dirname))
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+
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+ Rt = Rs + tc # cm
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+
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+ print "Wl = %.2f, Rs = %.2f, tc = %.2f, Rt = %.2f" % (wl, Rs, tc, Rt)
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+
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+ ms = 1.0 + 40.0j
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+ for i, fname in enumerate(files):
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+ print "Calculating spectra for file '%s'..." % (fname)
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+
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+ basename = os.path.splitext(fname)[0]
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+
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+ nvalues = np.loadtxt('%s/%s' % (dirname, fname))*1.0 + 1e-11j
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+
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+ tl = tc/len(nvalues) # cm
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+ r = [Rs]
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+
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+ for i in range(len(nvalues)):
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+ r += [r[i] + tl]
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+
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+ x = np.ones((1, len(nvalues) + 1), dtype = np.float64)
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+ m = np.ones((1, len(nvalues) + 1), dtype = np.complex128)
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+
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+ x[0] = 2.0*np.pi*np.array(r, dtype = np.float64)/wl
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+ m[0] = np.array([ms] + nvalues[:, 1].tolist(), dtype = np.complex128)
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+
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+ factor = 2
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+ comment='PEC-'+basename
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+ WL_units='cm'
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+ flow_total = 39
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+ #flow_total = 0
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+ #crossplane='XZ'
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+ crossplane='YZ'
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+ #crossplane='XY'
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+
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+ # Options to plot: Eabs, Habs, Pabs, angleEx, angleHy
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+ field_to_plot='Pabs'
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+ #field_to_plot='Eabs'
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+ #field_to_plot='angleEx'
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+ fieldplot(x[0],m[0], wl, comment, WL_units, crossplane, field_to_plot, npts,
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+ factor, flow_total, pl=0, outline_width=0.1)
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+
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+
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+ print "Done!!"
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+
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