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- #!/usr/bin/env python
- # -*- coding: UTF-8 -*-
- #
- # Copyright (C) 2009-2015 Ovidio Peña Rodríguez <ovidio@bytesfall.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 the following reference:
- # [1] O. Pena and U. Pal, "Scattering of electromagnetic radiation by
- # a multilayered sphere," Computer Physics Communications,
- # vol. 180, Nov. 2009, pp. 2348-2354.
- #
- # You should have received a copy of the GNU General Public License
- # along with this program. If not, see <http://www.gnu.org/licenses/>.
- # This test case calculates the electric field along three
- # points, for an spherical silver nanoparticle embedded in glass.
- # Refractive index values correspond to a wavelength of
- # 400 nm. Maximum of the surface plasmon resonance (and,
- # hence, of electric field) is expected under those
- # conditions.
- from scattnlay import fieldnlay
- import numpy as np
- x = np.ones((1, 2), dtype = np.float64)
- x[0, 0] = 2.0*np.pi*0.05/1.064
- x[0, 1] = 2.0*np.pi*0.06/1.064
- m = np.ones((1, 2), dtype = np.complex128)
- m[0, 0] = 1.53413/1.3205
- m[0, 1] = (0.565838 + 7.23262j)/1.3205
- coord = np.zeros((3, 3), dtype = np.float64)
- coord[0, 0] = x[0, 0]/2.0
- coord[1, 0] = (x[0, 0] + x[0, 1])/2.0
- coord[2, 0] = 1.5*x[0, 1]
- terms, E, H = fieldnlay(x, m, coord)
- Er = np.absolute(E)
- # |E|/|Eo|
- Eh = np.sqrt(Er[0, :, 0]**2 + Er[0, :, 1]**2 + Er[0, :, 2]**2)
- print x
- print m
- print np.vstack((coord[:, 0], Eh)).transpose()
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