update

examples/TiO2-comsol-compare.py

@@ -0,0 +1,143 @@
+#!/usr/bin/env python3
+# -*- coding: UTF-8 -*-
+#
+#    Copyright (C) 2021  Konstantin Ladutenko <kostyfisik@gmail.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/>.
+
+from scattnlay import mie
+import matplotlib.pyplot as plt
+import numpy as np
+from optical_constants import read_refractive_index_from_yaml as get_index
+
+def gauss(x, mu, sigma):
+    return 1/(sigma * np.sqrt(2 * np.pi)) * np.exp( - (x - mu)**2 / (2 * sigma**2))
+
+from_WL = 300
+to_WL = 1100
+WL_points= 100
+WLs = np.linspace(from_WL, to_WL, WL_points)
+
+from_r = 40/2.
+to_r =80/2.
+r_points = 20
+all_r = np.linspace(from_r, to_r, r_points)
+r_mean = 58.3/2.
+# r_mean = 50/2.
+r_std = 6.3/2.
+r_weights = gauss(all_r, r_mean,r_std)/len(all_r)
+
+plt.plot(all_r, r_weights )
+plt.xlabel("R, nm")
+plt.ylabel("amount")
+
+index_SiO2 = get_index("refractiveindex_info/SiO2-Gao.yml", WLs, units='nm')
+# index_Au = get_index("refractiveindex_info/Au-McPeak.yml", WLs, units='nm')
+index_Au = get_index("refractiveindex_info/Au-Johnson.yml", WLs, units='nm')
+index_TiO2 = get_index("r"
+                       "efractiveindex_info/TiO2-Sarkar.yml", WLs, units='nm')
+
+index_SiO2 *= 0; index_SiO2 += 1.45
+index_TiO2[:,1] += 0.0j
+# index_Au[:,1] += 1.5j
+
+x = np.ones((3), dtype = np.float64)
+m = np.ones((3), dtype = np.complex128)
+
+core_r = 5
+inner_shell_h = 10+20
+outer_shell_h = 10
+host_media = 1.33
+
+Qext_core_shell = np.zeros(len(WLs))
+Qext_3l = np.zeros(len(WLs))
+
+for i in range(len(WLs)):
+    WL = WLs[i]
+    for j in range(len(all_r)):
+        # core_r = all_r[j]
+        # weight = r_weights[j]
+        weight = 1/len(r_weights)
+        # print(core_r)
+        x = host_media*2.0*np.pi/WL*np.array([core_r,
+                                   core_r+inner_shell_h,
+                                   core_r+inner_shell_h+outer_shell_h])
+        m = np.array([index_SiO2[i][1], index_Au[i][1],
+                      index_TiO2[i][1]]
+                     )/host_media
+        # print(x, m)
+        mie.SetLayersSize(x)
+        mie.SetLayersIndex(m)
+        mie.RunMieCalculation()
+        Qext_3l[i] += mie.GetQext()*weight
+
+        x = host_media*2.0*np.pi/WL*np.array([core_r,
+                          core_r+inner_shell_h])
+        m = np.array([index_SiO2[i][1], index_Au[i][1]])/host_media
+        mie.SetLayersSize(x)
+        mie.SetLayersIndex(m)
+        mie.RunMieCalculation()
+        Qext_core_shell[i] += mie.GetQext()*weight
+
+comsol_spectra = np.array([[0.420000000000000,2.35836000000000e-15],
+                  [0.440000000000000,2.27000000000000e-15],
+                  [0.460000000000000,2.21146900000000e-15],
+                  [0.480000000000000,2.21744500000000e-15],
+                  [0.500000000000000,2.49989500000000e-15],
+                  [0.520000000000000,3.36257000000000e-15],
+                  [0.540000000000000,3.88983000000000e-15],
+                  [0.560000000000000,4.03982000000000e-15],
+                  [0.580000000000000,3.23889000000000e-15],
+                  [0.600000000000000,3.01499000000000e-15],
+                  [0.620000000000000,2.13147000000000e-15],
+                  [0.640000000000000,9.02930000000000e-16],
+                  [0.660000000000000,4.49688000000000e-16],
+                  [0.680000000000000,2.93514000000000e-16],
+                  [0.700000000000000,2.19381000000000e-16],
+                  [0.720000000000000,1.85272000000000e-16],
+                  [0.740000000000000,1.74517000000000e-16],
+                  [0.760000000000000,1.54702000000000e-16],
+                  [0.780000000000000,1.51191000000000e-16],
+                  [0.800000000000000,1.58785200000000e-16],
+                  [0.820000000000000,1.74967600000000e-16 ]  ])
+
+fig, axs2 = plt.subplots(1,1)#, sharey=True, sharex=True)
+# axs2.plot(WLs, Qext_3l, color="purple")
+axs2.plot(WLs, Qext_core_shell, color="lime", label="Mie, layered")
+axs2.plot(comsol_spectra[:,0]*1000, comsol_spectra[:,1]/np.pi/(35e-9**2)*3, color="black", label="Comsol, \nSiO2 with Au NP coating")
+axs2.legend()
+axs2.set_xlabel("WL, nm")
+axs2.set_ylabel("Extinction, a.u.")
+# axs2 = axs.twinx()
+# axs2.plot(np.array(core_r_vec)*2,an_vec[:,0],"b.",lw=0.8, markersize=1.9,label="$a_0$")
+# axs2.plot(np.array(core_r_vec)*2,bn_vec[:,0],"b-", markersize=1.9,label="$b_0$")
+# axs2.plot(np.array(core_r_vec)*2,an_vec[:,1],"g.",lw=0.8, markersize=1.9,label="$a_1$")
+# axs2.plot(np.array(core_r_vec)*2,bn_vec[:,1],"g-", markersize=1.9,label="$b_1$")
+# axs2.legend(loc="upper right")
+# axs2.tick_params('y', colors='black')
+# axs2.set_ylim(0,1)
+# axs2.set_ylabel("Mie",color="black")
+plt.savefig("spectra.pdf",pad_inches=0.02, bbox_inches='tight')
+plt.show()
+plt.clf()
+plt.close()

examples/calc-size-averaged-Qext.py

@@ -0,0 +1,159 @@
+#!/usr/bin/env python3
+# -*- coding: UTF-8 -*-
+#
+#    Copyright (C) 2021  Konstantin Ladutenko <kostyfisik@gmail.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/>.
+
+from scattnlay import mie
+import matplotlib.pyplot as plt
+import numpy as np
+from optical_constants import read_refractive_index_from_yaml as get_index
+
+def gauss(x, mu, sigma):
+    return 1/(sigma * np.sqrt(2 * np.pi)) * np.exp( - (x - mu)**2 / (2 * sigma**2))
+
+fill_factor = 0.8
+
+from_WL = 300
+to_WL = 1100
+WL_points= 100
+WLs = np.linspace(from_WL, to_WL, WL_points)
+
+r_points = 200
+
+from_r = 40/2.
+to_r =80/2.
+all_r = np.linspace(from_r, to_r, r_points)
+r_mean = 58.3/2.
+r_std = 6.3/2.
+
+
+# from_r = 1.
+# to_r =15.
+# all_r = np.linspace(from_r, to_r, r_points)
+# r_mean = 6
+# r_std = 2
+
+core_r = 30
+inner_shell_h = 8
+outer_shell_h = 10
+host_media = 1.33
+
+r_weights = gauss(all_r, r_mean,r_std)/len(all_r)
+
+plt.plot(all_r, r_weights )
+plt.xlabel("R, nm")
+plt.ylabel("amount")
+
+index_SiO2 = get_index("refractiveindex_info/SiO2-Gao.yml", WLs, units='nm')
+# index_Au = get_index("refractiveindex_info/Au-McPeak.yml", WLs, units='nm')
+index_Au = get_index("refractiveindex_info/Au-Johnson.yml", WLs, units='nm')
+index_TiO2 = get_index("refractiveindex_info/TiO2-Sarkar.yml", WLs, units='nm')
+
+# index_TiO2[:,1] += 0.5j
+# index_Au[:,1] = index_Au[:,1]* fill_factor + (1-fill_factor)
+
+print("Au index before correction, max = ", np.max(np.imag(index_Au[:,1])))
+# Taking into account gold free electrons damping
+# contributed by surface scattering and bulk dumping
+# See eq 1 in [1] -> doi: https://doi.org/10.1186/s11671-018-2670-7
+eps_exp = index_Au[:,1]**2
+c=299792458  # speed of light
+h= 4.135667516e-15  # eV*s, Planck constant
+w = h*c/(WLs*1e-9)  # eV, frequency
+w_p =8.55  # eV, gold plasmon frequency
+g_b = 18.4e-3  # eV, bulk dumping
+v_f = 1.4e6  # m/s, Fermi velocity of electrons in gold
+A = 1.33  # fit parameter for 16 nm gold shell, see Table 2 in [1]
+L_b = (4.*((core_r+inner_shell_h)**3 - core_r**3)/
+       (3.*((core_r+inner_shell_h)**2 + core_r**2)))
+# g_s = v_f/L_b  # eq 2 in [1]
+g_s = h*A*v_f/(inner_shell_h*1e-9)  # eq 4 in [1]
+# g_b *= 0.2
+# g_s *= 0.5
+eps_Au = (eps_exp
+          +
+          w_p**2 / ( w * (w + 1j*g_b) )
+          -
+          w_p**2 / ( w * (w + 1j*(g_b+g_s)) )
+          )
+# index_Au[:,1] = np.sqrt(eps_Au)
+index_Au[:,1] += 1.6j
+print(f"L_b={L_b}")
+# print(w)
+print(f"g_s={g_s}, g_b={g_b} ")
+print("Au index after, max = ", np.max(np.imag(index_Au[:,1])))
+x = np.ones((3), dtype = np.float64)
+m = np.ones((3), dtype = np.complex128)
+
+
+Qext_core_shell = np.zeros(len(WLs))
+Qext_3l = np.zeros(len(WLs))
+
+for i in range(len(WLs)):
+    WL = WLs[i]
+    for j in range(len(all_r)):
+        core_r = all_r[j]
+        # inner_shell_h = all_r[j]
+        weight = r_weights[j]
+        # print(core_r)
+        x = host_media*2.0*np.pi/WL*np.array([core_r,
+                                   core_r+inner_shell_h,
+                                   core_r+inner_shell_h+outer_shell_h])
+        m = np.array([index_SiO2[i][1], index_Au[i][1],
+                      index_TiO2[i][1]]
+                     )/host_media
+        # print(x, m)
+        mie.SetLayersSize(x)
+        mie.SetLayersIndex(m)
+        mie.RunMieCalculation()
+        Qext_3l[i] += mie.GetQext()*weight
+
+        x = host_media*2.0*np.pi/WL*np.array([core_r,
+                          core_r+inner_shell_h])
+        m = np.array([index_SiO2[i][1], index_Au[i][1]])/host_media
+        mie.SetLayersSize(x)
+        mie.SetLayersIndex(m)
+        mie.RunMieCalculation()
+        Qext_core_shell[i] += mie.GetQext()*weight
+
+
+fig, axs2 = plt.subplots(1,1)#, sharey=True, sharex=True)
+axs2.plot(WLs, Qext_3l, color="purple")
+axs2.plot(WLs, Qext_core_shell, color="lime")
+axs2.set_xlabel("WL, nm")
+axs2.set_ylabel("Extinction, a.u.")
+# axs2 = axs.twinx()
+# axs2.plot(np.array(core_r_vec)*2,an_vec[:,0],"b.",lw=0.8, markersize=1.9,label="$a_0$")
+# axs2.plot(np.array(core_r_vec)*2,bn_vec[:,0],"b-", markersize=1.9,label="$b_0$")
+# axs2.plot(np.array(core_r_vec)*2,an_vec[:,1],"g.",lw=0.8, markersize=1.9,label="$a_1$")
+# axs2.plot(np.array(core_r_vec)*2,bn_vec[:,1],"g-", markersize=1.9,label="$b_1$")
+# axs2.legend(loc="upper right")
+# axs2.tick_params('y', colors='black')
+# axs2.set_ylim(0,1)
+# axs2.set_ylabel("Mie",color="black")
+plt.savefig("spectra.pdf",pad_inches=0.02, bbox_inches='tight')
+plt.show()
+plt.clf()
+plt.close()

examples/refractiveindex_info/Au-Johnson.yml

@@ -0,0 +1,58 @@
+# this file is part of refractiveindex.info database
+# refractiveindex.info database is in the public domain
+# copyright and related rights waived via CC0 1.0
+
+REFERENCES: "P. B. Johnson and R. W. Christy. Optical constants of the noble metals, <a href=\"https://doi.org/10.1103/PhysRevB.6.4370\"><i>Phys. Rev. B</i> <b>6</b>, 4370-4379 (1972)</a>"
+COMMENTS: "Room temperature"
+DATA:
+  - type: tabulated nk
+    data: |
+        0.1879 1.28 1.188
+        0.1916 1.32 1.203
+        0.1953 1.34 1.226
+        0.1993 1.33 1.251
+        0.2033 1.33 1.277
+        0.2073 1.30 1.304
+        0.2119 1.30 1.350
+        0.2164 1.30 1.387
+        0.2214 1.30 1.427
+        0.2262 1.31 1.460
+        0.2313 1.30 1.497
+        0.2371 1.32 1.536
+        0.2426 1.32 1.577
+        0.2490 1.33 1.631
+        0.2551 1.33 1.688
+        0.2616 1.35 1.749
+        0.2689 1.38 1.803
+        0.2761 1.43 1.847
+        0.2844 1.47 1.869
+        0.2924 1.49 1.878
+        0.3009 1.53 1.889
+        0.3107 1.53 1.893
+        0.3204 1.54 1.898
+        0.3315 1.48 1.883
+        0.3425 1.48 1.871
+        0.3542 1.50 1.866
+        0.3679 1.48 1.895
+        0.3815 1.46 1.933
+        0.3974 1.47 1.952
+        0.4133 1.46 1.958
+        0.4305 1.45 1.948
+        0.4509 1.38 1.914
+        0.4714 1.31 1.849
+        0.4959 1.04 1.833
+        0.5209 0.62 2.081
+        0.5486 0.43 2.455
+        0.5821 0.29 2.863
+        0.6168 0.21 3.272
+        0.6595 0.14 3.697
+        0.7045 0.13 4.103
+        0.7560 0.14 4.542
+        0.8211 0.16 5.083
+        0.8920 0.17 5.663
+        0.9840 0.22 6.350
+        1.0880 0.27 7.150
+        1.2160 0.35 8.145
+        1.3930 0.43 9.519
+        1.6100 0.56 11.21
+        1.9370 0.92 13.78

examples/refractiveindex_info/Au-McPeak.yml

@@ -0,0 +1,150 @@
+# this file is part of refractiveindex.info database
+# refractiveindex.info database is in the public domain
+# copyright and related rights waived via CC0 1.0
+
+REFERENCES: "K. M. McPeak, S. V. Jayanti, S. J. P. Kress, S. Meyer, S. Iotti, A. Rossinelli, and D. J. Norris. Plasmonic films can easily be better: Rules and recipes, <a href=\"https://doi.org/10.1021/ph5004237\"><i>ACS Photonics</i> <b>2</b>, 326-333 (2015)</a>"
+COMMENTS: "Thermally evaporated Au at 10 Å/s with base pressure of 3e-8 Torr, template stripped from Si wafer"
+DATA:
+  - type: tabulated nk
+    data: |
+        0.3 1.699838715 1.973157788
+        0.31 1.746948702 1.974499878
+        0.32 1.782941044 1.959795593
+        0.33 1.804652963 1.931950392
+        0.34 1.804621334 1.896796816
+        0.35 1.763712432 1.870684779
+        0.36 1.713434851 1.887670254
+        0.37 1.689202065 1.922090949
+        0.38 1.678059067 1.948381952
+        0.39 1.672504217 1.966512231
+        0.4 1.665616091 1.973924254
+        0.41 1.653911114 1.975227068
+        0.42 1.63743714 1.970304643
+        0.43 1.612343317 1.959477219
+        0.44 1.581523054 1.940313163
+        0.45 1.538326354 1.910745397
+        0.46 1.475285274 1.872315849
+        0.47 1.386263242 1.827683172
+        0.48 1.252905499 1.782097694
+        0.49 1.064360219 1.76786953
+        0.5 0.848474841 1.828280492
+        0.51 0.661635502 1.964525779
+        0.52 0.52912664 2.129735899
+        0.53 0.438041087 2.294990195
+        0.54 0.372502061 2.451664289
+        0.55 0.323930966 2.597158307
+        0.56 0.284960267 2.738978341
+        0.57 0.254069233 2.871855006
+        0.58 0.228936734 2.999518633
+        0.59 0.207122197 3.1213458
+        0.6 0.188789629 3.241703491
+        0.61 0.172726107 3.356759495
+        0.62 0.160071695 3.465634566
+        0.63 0.14636792 3.577628204
+        0.64 0.135417727 3.685964997
+        0.65 0.125499436 3.792327795
+        0.66 0.117832095 3.896137113
+        0.67 0.111117685 3.999543366
+        0.68 0.105744888 4.102704228
+        0.69 0.101509306 4.205033191
+        0.7 0.098607898 4.305081128
+        0.71 0.097790271 4.403812319
+        0.72 0.098623269 4.499191766
+        0.73 0.096903666 4.59580138
+        0.74 0.099463321 4.687205239
+        0.75 0.098537395 4.78107829
+        0.76 0.099206649 4.872354868
+        0.77 0.101706737 4.958865219
+        0.78 0.101315225 5.051560628
+        0.79 0.103067755 5.148069829
+        0.8 0.10422723 5.223682926
+        0.81 0.105937788 5.313023886
+        0.82 0.104338656 5.407391844
+        0.83 0.104534544 5.49244276
+        0.84 0.107001078 5.577046641
+        0.85 0.111012574 5.659268839
+        0.86 0.11076329 5.749197205
+        0.87 0.112038779 5.830570529
+        0.88 0.114173034 5.912954886
+        0.89 0.116004573 5.992867182
+        0.9 0.116828465 6.081993825
+        0.91 0.116997234 6.163820922
+        0.92 0.11945701 6.241575921
+        0.93 0.120635837 6.328550624
+        0.94 0.122558964 6.410383818
+        0.95 0.124002721 6.491793025
+        0.96 0.123935366 6.573991175
+        0.97 0.126244253 6.662877577
+        0.98 0.127974627 6.73805443
+        0.99 0.129942772 6.819155749
+        1 0.132311724 6.904527963
+        1.01 0.133907614 6.978318655
+        1.02 0.135401137 7.061609835
+        1.03 0.138148809 7.141574413
+        1.04 0.137937636 7.222466808
+        1.05 0.139246667 7.302149658
+        1.06 0.134049061 7.406616579
+        1.07 0.135717763 7.48280825
+        1.08 0.140363062 7.556831465
+        1.09 0.138686104 7.637030433
+        1.1 0.138418628 7.719336741
+        1.11 0.139442944 7.79996438
+        1.12 0.141677831 7.874202982
+        1.13 0.141308241 7.960965269
+        1.14 0.140235564 8.050382973
+        1.15 0.142817756 8.114887363
+        1.16 0.146729336 8.201495565
+        1.17 0.152747848 8.26754691
+        1.18 0.149693183 8.350413645
+        1.19 0.147906483 8.443510901
+        1.2 0.149395088 8.515005513
+        1.21 0.151984867 8.589999965
+        1.22 0.153423422 8.666864413
+        1.23 0.153670698 8.744347585
+        1.24 0.157748208 8.81753279
+        1.25 0.159662147 8.900982642
+        1.26 0.165494236 8.987624177
+        1.27 0.159382324 9.068759713
+        1.28 0.163849184 9.146521008
+        1.29 0.166211578 9.226192405
+        1.3 0.166156462 9.303580384
+        1.31 0.170115488 9.372456417
+        1.32 0.169795214 9.445201449
+        1.33 0.174809869 9.530926424
+        1.34 0.176209118 9.61244244
+        1.35 0.179585571 9.687582308
+        1.36 0.177483381 9.769365402
+        1.37 0.184295562 9.839357949
+        1.38 0.186297714 9.916385775
+        1.39 0.190837556 9.992267959
+        1.4 0.191102283 10.07156989
+        1.41 0.194361931 10.14138928
+        1.42 0.205426553 10.22263176
+        1.43 0.208361137 10.32150252
+        1.44 0.206557078 10.37509835
+        1.45 0.208044 10.46581494
+        1.46 0.205758558 10.54050931
+        1.47 0.212405614 10.6421387
+        1.48 0.216697642 10.70593097
+        1.49 0.219902453 10.78046182
+        1.5 0.215398722 10.85893165
+        1.51 0.21956893 10.91137986
+        1.52 0.222004156 11.00587506
+        1.53 0.230589098 11.08617027
+        1.54 0.235210701 11.16849695
+        1.55 0.238229889 11.26307034
+        1.56 0.236761828 11.31706924
+        1.57 0.235275342 11.38092063
+        1.58 0.240819258 11.44281407
+        1.59 0.246290147 11.53172402
+        1.6 0.243652913 11.64299647
+        1.61 0.25211538 11.70912303
+        1.62 0.248830057 11.78354431
+        1.63 0.264448459 11.86507198
+        1.64 0.258451056 11.92798378
+        1.65 0.265882655 12.01168987
+        1.66 0.278561249 12.06969744
+        1.67 0.278188678 12.1875916
+        1.68 0.28090035 12.2404618
+        1.69 0.290244511 12.34683125
+        1.7 0.316481841 12.37053599

examples/refractiveindex_info/SiO2-Gao.yml

@@ -0,0 +1,509 @@
+# this file is part of refractiveindex.info database
+# refractiveindex.info database is in the public domain
+# copyright and related rights waived via CC0 1.0
+
+REFERENCES: "L. Gao, F. Lemarchand, M. Lequime. Refractive index determination of SiO<sub>2</sub> layer in the UV/Vis/NIR range: spectrophotometric reverse engineering on single and bi-layer designs, <a href=\"https://doi.org/10.2971/jeos.2013.13010\"><i>J. Europ. Opt. Soc. Rap. Public.</i> <b>8</b>, 13010 (2013)</a> (Numerical data kindly provided by F. Lemarchand)"
+COMMENTS: "300-nm monolayer deposited on fused silica using the ion assistance electronic beam deposition technique."
+DATA:
+  - type: tabulated nk
+    data: |
+        0.252 1.523846 0.001211
+        0.254 1.522945 0.001171
+        0.256 1.522066 0.001131
+        0.258 1.521208 0.001093
+        0.260 1.520370 0.001055
+        0.262 1.519552 0.001019
+        0.264 1.518753 0.000983
+        0.266 1.517972 0.000949
+        0.268 1.517209 0.000915
+        0.270 1.516463 0.000882
+        0.272 1.515734 0.000850
+        0.274 1.515021 0.000819
+        0.276 1.514325 0.000789
+        0.278 1.513643 0.000759
+        0.280 1.512977 0.000730
+        0.282 1.512325 0.000702
+        0.284 1.511687 0.000675
+        0.286 1.511063 0.000649
+        0.288 1.510452 0.000623
+        0.290 1.509854 0.000598
+        0.292 1.509268 0.000574
+        0.294 1.508695 0.000550
+        0.296 1.508134 0.000527
+        0.298 1.507584 0.000505
+        0.300 1.507046 0.000483
+        0.302 1.506518 0.000462
+        0.304 1.506002 0.000441
+        0.306 1.505495 0.000421
+        0.308 1.504999 0.000402
+        0.310 1.504512 0.000383
+        0.312 1.504035 0.000365
+        0.314 1.503568 0.000348
+        0.316 1.503109 0.000331
+        0.318 1.502660 0.000314
+        0.320 1.502219 0.000298
+        0.322 1.501786 0.000283
+        0.324 1.501361 0.000268
+        0.326 1.500945 0.000253
+        0.328 1.500536 0.000240
+        0.330 1.500135 0.000226
+        0.332 1.499742 0.000213
+        0.334 1.499355 0.000200
+        0.336 1.498976 0.000188
+        0.338 1.498603 0.000177
+        0.340 1.498238 0.000166
+        0.342 1.497878 0.000155
+        0.344 1.497525 0.000144
+        0.346 1.497179 0.000135
+        0.348 1.496838 0.000125
+        0.350 1.496504 0.000116
+        0.352 1.496175 0.000107
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+        0.364 1.494316 0.000063
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+        0.368 1.493738 0.000051
+        0.370 1.493455 0.000045
+        0.372 1.493177 0.000040
+        0.374 1.492904 0.000036
+        0.376 1.492635 0.000031
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+        0.384 1.491601 0.000016
+        0.386 1.491353 0.000014
+        0.388 1.491108 0.000011
+        0.390 1.490867 0.000009
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+        1.238 1.469407 0.000000
+        1.240 1.469400 0.000000
+        1.242 1.469392 0.000000
+        1.244 1.469384 0.000000
+        1.246 1.469377 0.000000
+        1.248 1.469369 0.000000
+        1.250 1.469362 0.000000

examples/refractiveindex_info/TiO2-Sarkar.yml

@@ -0,0 +1,987 @@
+# this file is part of refractiveindex.info database
+# refractiveindex.info database is in the public domain
+# copyright and related rights waived via CC0 1.0
+
+REFERENCES: "S. Sarkar, V. Gupta, M. Kumar, J. Schubert, P.T. Probst, J. Joseph, T.A.F. König, Hybridized guided-mode resonances via colloidal plasmonic self-assembled grating, <a href=\"https://doi.org/10.1021/acsami.8b20535\"><i>ACS Appl. Mater. Interfaces</i>, <b>11</b>, 13752-13760 (2019)</a><br>(Numerical data kindly provided by Dr. Tobias König)"
+COMMENTS: "Titanium(IV) oxide (Titanium dioxide, TiO<sub>2</sub>) thin film (thickness 200 nm) on glass substrate."
+DATA:
+  - type: tabulated nk
+    data: |
+        0.3000 2.809982 0.592784
+        0.3010 2.813419 0.577750
+        0.3020 2.816447 0.562667
+        0.3030 2.819065 0.547550
+        0.3040 2.821271 0.532415
+        0.3050 2.823066 0.517277
+        0.3060 2.824450 0.502151
+        0.3070 2.825424 0.487053
+        0.3080 2.825990 0.471999
+        0.3090 2.826151 0.457002
+        0.3100 2.825911 0.442080
+        0.3110 2.825273 0.427245
+        0.3120 2.824241 0.412513
+        0.3130 2.822823 0.397898
+        0.3140 2.821022 0.383415
+        0.3150 2.818847 0.369075
+        0.3160 2.816303 0.354894
+        0.3170 2.813400 0.340882
+        0.3180 2.810145 0.327054
+        0.3190 2.806546 0.313421
+        0.3200 2.802613 0.299994
+        0.3210 2.798357 0.286784
+        0.3220 2.793785 0.273802
+        0.3230 2.788909 0.261057
+        0.3240 2.783740 0.248560
+        0.3250 2.778289 0.236318
+        0.3260 2.772566 0.224341
+        0.3270 2.766583 0.212636
+        0.3280 2.760352 0.201211
+        0.3290 2.753886 0.190071
+        0.3300 2.747194 0.179225
+        0.3310 2.740291 0.168676
+        0.3320 2.733188 0.158431
+        0.3330 2.725897 0.148493
+        0.3340 2.718431 0.138869
+        0.3350 2.710803 0.129560
+        0.3360 2.703024 0.120570
+        0.3370 2.695107 0.111903
+        0.3380 2.687065 0.103560
+        0.3390 2.678910 0.095544
+        0.3400 2.670654 0.087855
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+        0.3530 2.559774 0.017800
+        0.3540 2.551405 0.014672
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+        0.3560 2.534941 0.009348
+        0.3570 2.526875 0.007147
+        0.3580 2.518941 0.005249
+        0.3590 2.511155 0.003650
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+        0.3610 2.496109 0.001333
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+        0.3630 2.481942 0.000165
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