Fix missing import in finiterectlat-scatter.py
[qpms.git] / misc / infiniterectlat-scatter.py
blob116d7b893acf8a030fe01cab033b9c1af0828fd0
1 #!/usr/bin/env python3
3 import math
4 pi = math.pi
5 from qpms.argproc import ArgParser, annotate_pdf_metadata
7 ap = ArgParser(['rectlattice2d', 'single_particle', 'single_lMax', 'omega_seq_real_ng', 'planewave'])
8 ap.add_argument("-o", "--output", type=str, required=False, help='output path (if not provided, will be generated automatically)')
9 ap.add_argument("-O", "--plot-out", type=str, required=False, help="path to plot output (optional)")
10 ap.add_argument("-P", "--plot", action='store_true', help="if -p not given, plot to a default path")
11 #ap.add_argument("-g", "--save-gradually", action='store_true', help="saves the partial result after computing each irrep")
14 a=ap.parse_args()
16 import logging
17 logging.basicConfig(format='%(asctime)s %(message)s', level=logging.INFO)
19 import numpy as np
20 import qpms
21 from qpms.qpms_p import cart2sph, sph2cart, sph_loccart2cart, sph_loccart_basis
22 import warnings
23 from qpms.cybspec import BaseSpec
24 from qpms.cytmatrices import CTMatrix, TMatrixGenerator
25 from qpms.qpms_c import Particle, pgsl_ignore_error
26 from qpms.cymaterials import EpsMu, EpsMuGenerator, LorentzDrudeModel, lorentz_drude
27 from qpms.cycommon import DebugFlags, dbgmsg_enable
28 from qpms import FinitePointGroup, ScatteringSystem, BesselType, eV, hbar
29 eh = eV/hbar
31 dbgmsg_enable(DebugFlags.INTEGRATION)
33 px, py = a.period
35 particlestr = ("sph" if a.height is None else "cyl") + ("_r%gnm" % (a.radius*1e9))
36 if a.height is not None: particlestr += "_h%gnm" % (a.height * 1e9)
37 defaultprefix = "%s_p%gnmx%gnm_m%s_bg%s%g_θ(%g_%g)π_ψ%gπ_χ%gπ_f%s_L%d" % (
38 particlestr, px*1e9, py*1e9, str(a.material), str(a.background), a.phi/pi, np.amin(a.theta)/pi, np.amax(a.theta)/pi, a.psi/pi, a.chi/pi, ap.omega_descr, a.lMax)
39 logging.info("Default file prefix: %s" % defaultprefix)
42 a1 = ap.direct_basis[0]
43 a2 = ap.direct_basis[1]
45 #Particle positions
46 orig_x = [0]
47 orig_y = [0]
48 orig_xy = np.stack(np.meshgrid(orig_x,orig_y),axis=-1)
50 bspec = BaseSpec(lMax = a.lMax)
51 # The parameters here should probably be changed (needs a better qpms_c.Particle implementation)
52 pp = Particle(orig_xy[0][0], ap.tmgen, bspec=bspec)
53 par = [pp]
56 ss, ssw = ScatteringSystem.create(par, ap.background_emg, ap.allomegas[0], latticebasis = ap.direct_basis)
59 ## Plane wave data
60 a.theta = np.array(a.theta)
61 dir_sph_list = np.stack((np.broadcast_to(1, a.theta.shape), a.theta, np.broadcast_to(a.phi, a.theta.shape)), axis=-1)
62 ,= math.sin(a.psi), math.cos(a.psi)
63 ,= math.sin(a.chi), math.cos(a.chi)
64 E_sph = (0.,*+ 1j**,*+ 1j**)
66 dir_cart_list = sph2cart(dir_sph_list)
67 E_cart_list = sph_loccart2cart(E_sph, dir_sph_list)
69 nfreq = len(ap.allomegas)
70 ndir = len(dir_sph_list)
72 k_cart_arr = np.empty((nfreq, ndir, 3), dtype=float)
73 wavenumbers = np.empty((nfreq,), dtype=float)
75 σ_ext_arr = np.empty((nfreq,ndir), dtype=float)
76 σ_scat_arr = np.empty((nfreq,ndir), dtype=float)
78 with pgsl_ignore_error(15): # avoid gsl crashing on underflow
79 for i, omega in enumerate(ap.allomegas):
80 if i != 0:
81 ssw = ss(omega)
82 if ssw.wavenumber.imag != 0:
83 warnings.warn("The background medium wavenumber has non-zero imaginary part. Don't expect meaningful results for cross sections.")
84 wavenumber = ssw.wavenumber.real
85 wavenumbers[i] = wavenumber
87 k_sph_list = np.array(dir_sph_list, copy=True)
88 k_sph_list[:,0] = wavenumber
90 k_cart_arr[i] = sph2cart(k_sph_list)
93 for j in range(ndir):
94 k_cart = k_cart_arr[i,j]
95 blochvector = (k_cart[0], k_cart[1], 0)
96 # the following two could be calculated only once, but probably not a big deal
97 LU = ssw.scatter_solver(k=blochvector)
98 ã = ss.planewave_full(k_cart=k_cart, E_cart=E_cart_list[j])
99 = ssw.apply_Tmatrices_full(ã)
100 f = LU()
102 σ_ext_arr[i,j] = -np.vdot(ã, f).real/wavenumber**2
103 translation_matrix = ssw.translation_matrix_full(blochvector=blochvector) + np.eye(ss.fecv_size)
104 σ_scat_arr[i,j] = np.vdot(f,np.dot(translation_matrix, f)).real/wavenumber**2
106 σ_abs_arr = σ_ext_arr - σ_scat_arr
108 outfile = defaultprefix + ".npz" if a.output is None else a.output
109 np.savez(outfile, meta={**vars(a), 'qpms_version' : qpms.__version__()}, dir_sph=dir_sph_list, k_cart = k_cart_arr, omega = ap.allomegas, E_cart = E_cart_list, wavenumbers= wavenumbers, σ_ext=σ_ext_arr,σ_abs=σ_abs_arr,σ_scat=σ_scat_arr, unitcell_area=ss.unitcell_volume
111 logging.info("Saved to %s" % outfile)
114 if a.plot or (a.plot_out is not None):
115 import matplotlib
116 from matplotlib.backends.backend_pdf import PdfPages
117 matplotlib.use('pdf')
118 from matplotlib import pyplot as plt
119 from scipy.interpolate import griddata
121 plotfile = defaultprefix + ".pdf" if a.plot_out is None else a.plot_out
122 with PdfPages(plotfile) as pdf:
123 ipm = 'nearest'
124 sintheta = np.sin(a.theta)
125 if False: #len(ap.omega_ranges) != 0:
126 # angle plot ---------------------------------
127 fig = plt.figure(figsize=(210/25.4, 297/25.4))
128 vmax = max(np.amax(σ_ext_arr), np.amax(σ_scat_arr), np.amax(σ_abs_arr))
129 vmin = min(np.amin(σ_ext_arr), np.amin(σ_scat_arr), np.amin(σ_abs_arr))
131 ax = fig.add_subplot(311)
132 ax.pcolormesh(a.theta, ap.allomegas/eh, σ_ext_arr, vmin=vmin, vmax=vmax)
133 ax.set_xlabel('$\\theta$')
134 ax.set_ylabel('$\\hbar\\omega / \\mathrm{eV}$')
135 ax.set_title('$\\sigma_\\mathrm{ext}$')
137 ax = fig.add_subplot(312)
138 ax.pcolormesh(a.theta, ap.allomegas/eh, σ_scat_arr, vmin=vmin, vmax=vmax)
139 ax.set_xlabel('$\\theta$')
140 ax.set_ylabel('$\\hbar\\omega / \\mathrm{eV}$')
141 ax.set_title('$\\sigma_\\mathrm{scat}$')
143 ax = fig.add_subplot(313)
144 im = ax.pcolormesh(a.theta, ap.allomegas/eh, σ_abs_arr, vmin=vmin, vmax=vmax)
145 ax.set_xlabel('$\\theta$')
146 ax.set_ylabel('$\\hbar\\omega / \\mathrm{eV}$')
147 ax.set_title('$\\sigma_\\mathrm{abs}$')
150 fig.subplots_adjust(right=0.8)
151 fig.colorbar(im, cax = fig.add_axes([0.85, 0.15, 0.05, 0.7]))
153 pdf.savefig(fig)
154 plt.close(fig)
156 if len(ap.omega_ranges) != 0:
157 # "k-space" plot -----------------------------
158 domega = np.amin(np.diff(ap.allomegas))
159 dsintheta = np.amin(abs(np.diff(sintheta)))
160 dk = dsintheta * wavenumbers[0]
162 # target image grid
163 grid_y, grid_x = np.mgrid[ap.allomegas[0] : ap.allomegas[-1] : domega, np.amin(sintheta) * wavenumbers[-1] : np.amax(sintheta) * wavenumbers[-1] : dk]
164 imextent = (np.amin(sintheta) * wavenumbers[-1] / 1e6, np.amax(sintheta) * wavenumbers[-1] / 1e6, ap.allomegas[0] / eh, ap.allomegas[-1] / eh)
166 # source coordinates for griddata
167 ktheta = sintheta[None, :] * wavenumbers[:, None]
168 omegapoints = np.broadcast_to(ap.allomegas[:, None], ktheta.shape)
169 points = np.stack( (ktheta.flatten(), omegapoints.flatten()), axis = -1)
171 fig = plt.figure(figsize=(210/25.4, 297/25.4))
172 vmax = np.amax(σ_ext_arr)
174 ax = fig.add_subplot(311)
175 grid_z = griddata(points, σ_ext_arr.flatten(), (grid_x, grid_y), method = ipm)
176 ax.imshow(grid_z, extent = imextent, origin = 'lower', vmin = 0, vmax = vmax, aspect = 'auto', interpolation='none')
177 ax.set_xlabel('$k_\\theta / \\mathrm{\\mu m^{-1}}$')
178 ax.set_ylabel('$\\hbar\\omega / \\mathrm{eV}$')
179 ax.set_title('$\\sigma_\\mathrm{ext}$')
181 ax = fig.add_subplot(312)
182 grid_z = griddata(points, σ_scat_arr.flatten(), (grid_x, grid_y), method = ipm)
183 ax.imshow(grid_z, extent = imextent, origin = 'lower', vmin = 0, vmax = vmax, aspect = 'auto', interpolation='none')
184 ax.set_xlabel('$k_\\theta / \\mathrm{\\mu m^{-1}}$')
185 ax.set_ylabel('$\\hbar\\omega / \\mathrm{eV}$')
186 ax.set_title('$\\sigma_\\mathrm{scat}$')
188 ax = fig.add_subplot(313)
189 grid_z = griddata(points, σ_abs_arr.flatten(), (grid_x, grid_y), method = ipm)
190 im = ax.imshow(grid_z, extent = imextent, origin = 'lower', vmin = 0, vmax = vmax, aspect = 'auto', interpolation='none')
191 ax.set_xlabel('$k_\\theta / \\mathrm{\\mu m^{-1}}$')
192 ax.set_ylabel('$\\hbar\\omega / \\mathrm{eV}$')
193 ax.set_title('$\\sigma_\\mathrm{abs}$')
195 fig.subplots_adjust(right=0.8)
196 fig.colorbar(im, cax = fig.add_axes([0.85, 0.15, 0.05, 0.7]))
198 pdf.savefig(fig)
199 plt.close(fig)
201 for omega in ap.omega_singles:
202 i = np.searchsorted(ap.allomegas, omega)
204 fig = plt.figure()
205 fig.suptitle("%g eV" % (omega / eh))
206 ax = fig.add_subplot(111)
207 sintheta = np.sin(a.theta)
208 ax.plot(sintheta, σ_ext_arr[i]*1e12,label='$\sigma_\mathrm{ext}$')
209 ax.plot(sintheta, σ_scat_arr[i]*1e12, label='$\sigma_\mathrm{scat}$')
210 ax.plot(sintheta, σ_abs_arr[i]*1e12, label='$\sigma_\mathrm{abs}$')
211 ax.legend()
212 ax.set_xlabel('$\sin\\theta$')
213 ax.set_ylabel('$\sigma/\mathrm{\mu m^2}$')
215 pdf.savefig(fig)
216 plt.close(fig)
217 annotate_pdf_metadata(pdf)
218 exit(0)