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- #!/usr/bin/env python
- # -*- 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 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 in the
- # XY plane, for a silver nanoshell embedded in water.
- # Refractive index values correspond to the wavelength
- # where maximum of the surface plasmon resonance (and,
- # hence, of electric field) is expected.
- from scattnlay import fieldnlay
- import numpy as np
- n1 = 1.46
- nm = 1.0
- x = np.ones((1, 1), dtype = np.float64)
- x[0, 0] = 5.0
- m = np.ones((1, 1), dtype = np.complex128)
- m[0, 0] = n1/nm
- print "x =", x
- print "m =", m
- npts = 1001
- scan = np.linspace(-3.0*x[0, -1], 3.0*x[0, -1], npts)
- coordX, coordZ = np.meshgrid(scan, scan)
- coordX.resize(npts*npts)
- coordZ.resize(npts*npts)
- coordY = np.zeros(npts*npts, dtype = np.float64)
- terms, E, H = fieldnlay(x, m, coordX, coordY, coordZ)
- Er = np.absolute(E)
- # |E|/|Eo|
- Eh = np.sqrt(Er[0, :, 0]**2 + Er[0, :, 1]**2 + Er[0, :, 2]**2)
- result = np.vstack((coordX, coordY, coordZ, Eh)).transpose()
- try:
- import matplotlib.pyplot as plt
- from matplotlib import cm
- from matplotlib.colors import LogNorm
- min_tick = 0.5
- max_tick = 1.0
- edata = np.resize(Eh, (npts, npts)).transpose()
- fig = plt.figure()
- ax = fig.add_subplot(111)
- # Rescale to better show the axes
- scale_x = np.linspace(min(coordX), max(coordX), npts)
- scale_z = np.linspace(min(coordZ), max(coordZ), npts)
- # Define scale ticks
- min_tick = min(min_tick, np.amin(edata))
- max_tick = max(max_tick, np.amax(edata))
- scale_ticks = np.power(10.0, np.linspace(np.log10(min_tick), np.log10(max_tick), 6))
- #scale_ticks = np.linspace(min_tick, max_tick, 6)
- # Interpolation can be 'nearest', 'bilinear' or 'bicubic'
- cax = ax.imshow(edata, interpolation = 'nearest', cmap = cm.jet,
- origin = 'lower', vmin = min_tick, vmax = max_tick,
- extent = (min(scale_z), max(scale_z), min(scale_x), max(scale_x)),
- norm = LogNorm())
- # Add colorbar
- cbar = fig.colorbar(cax, ticks = [a for a in scale_ticks])
- cbar.ax.set_yticklabels(['%4.2g' % (a) for a in scale_ticks]) # vertically oriented colorbar
- pos = list(cbar.ax.get_position().bounds)
- fig.text(pos[0] - 0.02, 0.925, '|E|/|E$_0$|', fontsize = 14)
- plt.xlabel('Z')
- plt.ylabel('X')
- # This part draws the nanoshell
- from matplotlib import patches
- s1 = patches.Arc((0, 0), 2.0*x[0, 0], 2.0*x[0, 0], angle=0.0, zorder=2,
- theta1=0.0, theta2=360.0, linewidth=1, color='black')
- ax.add_patch(s1)
- # s2 = patches.Arc((0, 0), 2.0*x[0, 1], 2.0*x[0, 1], angle=0.0, zorder=2,
- # theta1=0.0, theta2=360.0, linewidth=1, color='#00fa9a')
- # ax.add_patch(s2)
- # End of drawing
- plt.draw()
- plt.show()
- plt.clf()
- plt.close()
- finally:
- np.savetxt("field-silica.txt", result, fmt = "%.5f")
- print result
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