From 679ee72bee36b8d17ff2e783e20c3c34a2bcf762 Mon Sep 17 00:00:00 2001 From: =?UTF-8?q?Marek=20Ne=C4=8Dada?= Date: Thu, 9 Dec 2021 11:19:19 +0200 Subject: [PATCH] Helper class to analyse results of finiterectlat-modes.py --- qpms/analysis.py | 132 +++++++++++++++++++++++++++++++++++++++++++++++ 1 file changed, 132 insertions(+) create mode 100644 qpms/analysis.py diff --git a/qpms/analysis.py b/qpms/analysis.py new file mode 100644 index 0000000..4d79e4b --- /dev/null +++ b/qpms/analysis.py @@ -0,0 +1,132 @@ +''' +Auxiliary functions to analyse results obtained using scripts in +the ../misc directory. + +This needs to be kept in sync with the scripts and qpms/argproc.py. +''' + +import numpy as np +import qpms +from qpms.qpms_c import Particle +from qpms.cytmatrices import CTMatrix, TMatrixGenerator +from qpms.cybspec import BaseSpec +from qpms.cymaterials import EpsMu, EpsMuGenerator, LorentzDrudeModel, lorentz_drude +from qpms.symmetries import point_group_info +from qpms import FinitePointGroup, ScatteringSystem, eV, hbar +eh = eV / hbar + +def cleanarray(a, atol=1e-8, copy=True, fullNaN=True): + a = np.array(a, copy=copy) + sieve = abs(a.real) < atol + a[sieve] = 1j * a[sieve].imag + sieve = abs(a.imag) < atol + a[sieve] = a[sieve].real + if fullNaN: + if np.all(a == 0): + a[...] = 0 + return a + +def nicerot(a, atol=1e-10, copy=True): + ''' + Gives an array a "nice" phase. + ''' + a = np.array(a, copy=copy) + i = np.argmax(abs(a)) + a = a / a[i] * abs(a[i]) + return a + +def _meta_matspec2emg(matspec): + if isinstance(matspec, (float, complex)): # number is interpreted as refractive index + return EpsMuGenerator(EpsMu(matspec**2)) + else: + return EpsMuGenerator(lorentz_drude[matspec]) + + +class FiniteRectLatModesAnalysis: + '''Recreates the scattering system structure from finiterectlat_modes.py''' + def __init__(self, data): + meta = data['meta'][()] + thegroup = 'D2h' if meta['D2'] else 'D4h' + Nx, Ny = meta['size'] + px, py = meta['period'] + orig_x = (np.arange(Nx/2) + (0 if (Nx % 2) else .5)) * px + orig_y = (np.arange(Ny/2) + (0 if (Ny % 2) else .5)) * py + orig_xy = np.stack(np.meshgrid(orig_x, orig_y), axis = -1) + bspec = BaseSpec(lMax = meta['lMax']) + nelem = len(bspec) + bg = _meta_matspec2emg(meta['background']) + fg = _meta_matspec2emg(meta['material']) + if meta.get('height', None) is None: + tmgen = TMatrixGenerator.sphere(bg, fg, meta['radius']) + else: + tmgen = TMatrixGenerator.cylinder(bg, fg, meta['radius'], meta['height'], lMax_extend=meta['lMax_extend']) + particles = [Particle(orig_xy[i], tmgen, bspec) for i in np.ndindex(orig_xy.shape[:-1])] + sym = FinitePointGroup(point_group_info[thegroup]) + self.ss, self.ssw = ScatteringSystem.create(particles, bg, meta['centre'] * eh, sym=sym) + ss1, ssw1 = ScatteringSystem.create([Particle([0,0,0], tmgen, bspec)], bg, meta['centre']*eh, sym=sym) + self.ss1, self.ssw1 = ss1, ssw1 + + # per-particle projectors/transformation to symmetry-adapted bases + fvcs1 = np.empty((nelem, nelem), dtype=complex) + y = 0 + iris1 = [] + for iri1 in range(ss1.nirreps): + for j in range(ss1.saecv_sizes[iri1]): + pvc1 = np.zeros((ss1.saecv_sizes[iri1],), dtype=complex) + pvc1[j] = 1 + fvcs1[y] = ss1.unpack_vector(pvc1, iri1) + fvcs1[y] = cleanarray(nicerot(fvcs1[y], copy=False), copy=False) + y += 1 + iris1.append(iri1) + + # Mapping between ss particles and grid positions; + positions = self.ss.positions.astype(np.float32) # cast to eliminate rounding errors + xpositions = np.unique(positions[:,0]) + assert(len(xpositions) == Nx) + ypositions = np.unique(positions[:,1]) + assert(len(ypositions == Ny)) + # particle positions as integer indices + posmap = np.empty((positions.shape[0],2), dtype=int) + #invposmap = np.empty((Nx, Ny), dtype=int) + for i, pos in enumerate(positions): + posmap[i,0] = np.searchsorted(xpositions, positions[i,0]) + posmap[i,1] = np.searchsorted(ypositions, positions[i,1]) + #invposmap[posmap[i,0], posmap[i, 1]] = i + + self.meta = meta + self.npzfile = data + self.eigval = data['eigval'] + self.neig = len(self.eigval) + self.eigvec = data['eigvec'] + self.residuals = data['residuals'] + self.ranktest_SV = data['ranktest_SV'] + self.iri = data['iri'][()] + self.bspec = bspec + self.nelem = nelem + self.Nx, self.Ny, self.px, self.py = Nx, Ny, px, py + self.posmap = posmap + self.fullvec_poffsets = nelem * np.arange(Nx*Ny) + self.fvcs1 = fvcs1 + self.iris1 = np.array(iris1) + + + def fullvec2grid(self, fullvec, swapxy=False): + arr = np.empty((self.Nx, self.Ny, self.nelem), dtype=complex) + for pi, offset in enumerate(self.fullvec_poffsets): + ix, iy = self.posmap[pi] + arr[ix, iy] = fullvec[offset:offset+self.nelem] + return np.swapaxes(arr, 0, 1) if swapxy else arr + + def saecv2grid(self, saecv, swapxy=False): + fullvec = self.ss.unpack_vector(saecv, iri=self.iri) + return self.fullvec2grid(fullvec, swapxy) + + def eigvec_asgrid(self, i, swapxy = False): + ''' + Returns i-th eigenmode as a (Nx, Ny, nelem)-shaped grid of excitation + coefficients. + ''' + if self.iri is not None: + return self.saecv2grid(self.eigvec[i], swapxy) + else: + return self.fullvec2grid(self.eigvec[i], swapxy)