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Mie_resonances_vs_Radius.gif (243 × 243 pixels, file size: 5.67 MB, MIME type: image/gif, looped, 202 frames, 30 s)

Summary

Description
English: Effect of a dielectric sphere (technically a disk, as the simulation is in 2D) on an incident plane wave as a function of the radius. The patterns you see flashing in are the Mie resonances. The incident plane wave is coming from the bottom.
Date
Source https://twitter.com/j_bertolotti/status/1388821332989775875
Author Jacopo Bertolotti
Permission
(Reusing this file)
https://twitter.com/j_bertolotti/status/1030470604418428929

Mathematica 12.0 code

\[Lambda]0 = 1.; k0 = 
 N[(2 \[Pi])/\[Lambda]0]; (*The wavelength in vacuum is set to 1, so all lengths are now in units of wavelengths*)
\[Delta] = \[Lambda]0/20; \[CapitalDelta] = 20*\[Lambda]0; (*Parameters for the grid*)
sourcef[x_, y_] := E^(I k0 y); (*Important! The source MUST be a solution of the Helmholtz equation in vacuum*)
\[Phi]in = Table[sourcef[x, y], {x, -\[CapitalDelta]/2, \[CapitalDelta]/ 2, \[Delta]}, {y, -\[CapitalDelta]/2, \[CapitalDelta]/ 2, \[Delta]}]; (*Discretized source*)
d = \[Lambda]0/1; (*typical scale of the absorbing layer*)
imn =  Table[5 I (E^-((x + \[CapitalDelta]/2)/d) + E^((x - \[CapitalDelta]/2)/d) + E^-((y + \[CapitalDelta]/2)/d) + E^((y - \[CapitalDelta]/2)/d)), {x, -\[CapitalDelta]/2, \[CapitalDelta]/2, \[Delta]}, {y, -\[CapitalDelta]/ 2, \[CapitalDelta]/ 2, \[Delta]}]; (*Imaginary part of the refractive index (used to emulate absorbing boundaries)*)
dim = Dimensions[\[Phi]in][[1]];
L = -1/\[Delta]^2*KirchhoffMatrix[GridGraph[{dim, dim}]]; (*Discretized Laplacian*)
r[t_] := (\[Lambda]0*3 - \[Delta]*5) Sin[\[Pi]/ 2 t]^2 + \[Delta]*5; (*The radius changes with the parameter t*)
frames = Table[
  n = Table[
     If[y^2 + x^2 <= r[t]^2, 2, 1], {x, -\[CapitalDelta]/ 2, \[CapitalDelta]/2, \[Delta]}, {y, -\[CapitalDelta]/ 2, \[CapitalDelta]/2, \[Delta]}] + imn; (*Matrix with the refractive index*)
  b = -(Flatten[n]^2 - 1) k0^2 Flatten[\[Phi]in]; (*Right-hand side of the equation we want to solve*)
  M = L + DiagonalMatrix[SparseArray[Flatten[n]^2 k0^2]]; (*Operator on the left-hand side of the equation we want to solve*)
  \[Phi]s = Partition[LinearSolve[M, b], dim]; (*Solve the linear system*)
  
  ImageAdd[
   ArrayPlot[
    Transpose[Abs[\[Phi]in + \[Phi]s]^2/ Max[Abs[\[Phi]in + \[Phi]s]^2]][[(4 d)/\[Delta] ;; (-4 d)/\[Delta], (4 d)/\[Delta] ;; (-4 d)/\[Delta]]], ColorFunction -> "AvocadoColors" , DataReversed -> True, 
    Frame -> False, PlotRange -> {0, 0.8}], ArrayPlot[Transpose@Re[(n - 1)/10] , DataReversed -> True , ColorFunctionScaling -> False, ColorFunction -> GrayLevel, Frame -> False]
   ](*Plot everything*)
  , {t, 0, 1, 1./100}];
ListAnimate[frames]

Licensing

I, the copyright holder of this work, hereby publish it under the following license:
Creative Commons CC-Zero This file is made available under the Creative Commons CC0 1.0 Universal Public Domain Dedication.
The person who associated a work with this deed has dedicated the work to the public domain by waiving all of their rights to the work worldwide under copyright law, including all related and neighboring rights, to the extent allowed by law. You can copy, modify, distribute and perform the work, even for commercial purposes, all without asking permission.

Captions

Plane wave incident on a dielectric sphere of varying radius.

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2 May 2021

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Date/TimeThumbnailDimensionsUserComment
current08:51, 4 May 2021Thumbnail for version as of 08:51, 4 May 2021243 × 243 (5.67 MB)BertoUploaded own work with UploadWizard

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