File:Optical fibres modes vs wavelength.gif

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Summary

Description
English: The number of modes allowed in an optical fibre depends on the fibre itself (radius and refractive index) and the wavelength you are using. (Showing only the energy distribution of TE modes for simplicity.)
Date
Source https://twitter.com/j_bertolotti/status/1320687090246496261
Author Jacopo Bertolotti
Permission
(Reusing this file)
https://twitter.com/j_bertolotti/status/1030470604418428929

Mathematica 12.1 code

(*Root-finding code idea from https://mathematica.stackexchange.com/questions/16439/find-all-roots-of-an-interpolating-function-solution-to-a-differential-equation/16444#16444*)
Clear[findAllRoots]
SyntaxInformation[findAllRoots] = {"LocalVariables" -> {"Plot", {2, 2}}, "ArgumentsPattern" -> {_, _, OptionsPattern[]}};
SetAttributes[findAllRoots, HoldAll];
Options[findAllRoots] = Join[{"ShowPlot" -> False, PlotRange -> All}, FilterRules[Options[Plot], Except[PlotRange]]];
findAllRoots[fn_, {l_, lmin_, lmax_}, opts : OptionsPattern[]] := Module[{pl, p, x, localFunction, brackets}, localFunction = ReleaseHold[Hold[fn] /. HoldPattern[l] :> x];
  If[lmin != lmax, pl = Plot[localFunction, {x, lmin, lmax}, Evaluate@FilterRules[Join[{opts}, Options[findAllRoots]], Options[Plot]]];
   p = Cases[pl, Line[{x__}] :> x, Infinity];
   If[OptionValue["ShowPlot"], Print[Show[pl, PlotLabel -> "Finding roots for this function", ImageSize -> 200, BaseStyle -> {FontSize -> 8}]]], p = {}];
  brackets = Map[First, Select[(*This Split trick pretends that two points on the curve are "equal" if the function values have _opposite _ sign.Pairs of such sign-changes form the brackets for the subsequent FindRoot*) Split[p, Sign[Last[#2]] == -Sign[Last[#1]] &], Length[#1] == 2 &], {2}];
  x /. Apply[FindRoot[localFunction == 0, {x, ##1}] &, brackets, {1}] /. x -> {}]
(*8*)
\[Lambda] =.;
k0[\[Lambda]_] := (2 \[Pi])/\[Lambda];
n0 = 1; n1 = 1.1; \[Mu]0 = 1; c = 1; \[Omega][\[Lambda]_] := k0[\[Lambda]] c;
r0 = 2;
\[Beta][\[Lambda]_, kz_] := Sqrt[k0[\[Lambda]]^2 n1^2 - kz^2];
\[Sigma][\[Lambda]_, kz_] := Sqrt[kz^2 - k0[\[Lambda]]^2 n0^2];
dispersionTE[\[Lambda]_, kz_] := BesselJ[1, \[Beta][\[Lambda], kz] r0]/(\[Beta][\[Lambda], kz] BesselJ[0, \[Beta][\[Lambda], kz] r0]) + BesselK[1, \[Sigma][\[Lambda], kz] r0]/(\[Sigma][\[Lambda], kz] BesselK[0, \[Sigma][\[Lambda], kz] r0]);
Er[r_, root_] := 0; H\[Phi][r_, root_] := 0;
E\[Phi][r_, root_] := Piecewise[{{-I (\[Omega][\[Lambda]] \[Mu]0 )/\[Beta][\[Lambda], kz] BesselJ[1, \[Beta][\[Lambda], kz] r], r < r0}, {I (\[Omega][\[Lambda]] \[Mu]0)/\[Sigma][\[Lambda], kz] BesselJ[0, \[Beta][\[Lambda], kz] r0]/ BesselK[0, \[Sigma][\[Lambda], kz] r0] BesselK[1, \[Sigma][\[Lambda], kz] r], r >= r0}}] /. {kz -> root};
Hr[r_, root_] := Piecewise[{{I  BesselJ[1, \[Beta][\[Lambda], kz] r], r < r0}, {-I \[Beta][\[Lambda], kz]/\[Sigma][\[Lambda], kz] BesselJ[0, \[Beta][\[Lambda], kz] r0]/ BesselK[0, \[Sigma][\[Lambda], kz] r0] BesselK[1, \[Sigma][\[Lambda], kz] r], r >= r0}}] /. {kz -> root};
Hz[r_, root_] := Piecewise[{{BesselJ[0, \[Beta][\[Lambda], kz] r], r < r0}, {BesselJ[0, \[Beta][\[Lambda], kz] r0]/ BesselK[0, \[Sigma][\[Lambda], kz] r0] BesselK[0, \[Sigma][\[Lambda], kz] r], r >= r0}}] /. {kz -> root};

modes = Table[
   rootsTE = findAllRoots[dispersionTE[\[Lambda], kz], {kz, 0, 25}];
   rootsTE = Sort[rootsTE[[Flatten@Position[Evaluate[dispersionTE[\[Lambda], #] & /@ rootsTE], _?(Abs[#] < 1 &)]]] ];
   Column[{
     Style[StringForm["TE modes. \!\(\*FractionBox[\(\[Lambda]\), \(R\)]\)=``", NumberForm[N[\[Lambda]/r0], {3, 2}]], Black, Bold, FontSize -> 14],
     GraphicsRow[
      Table[DensityPlot[Norm[Hz[Sqrt[x^2 + y^2], rootsTE[[j]]]]^2 + Norm[Hr[Sqrt[x^2 + y^2], rootsTE[[j]]]]^2 + Norm[E\[Phi][Sqrt[x^2 + y^2], rootsTE[[j]]]]^2, {x, -1.5 r0, 1.5 r0}, {y, -1.5 r0, 1.5 r0}, PlotPoints -> 50, PlotRange -> All, ColorFunction -> "AvocadoColors", Frame -> False], {j, 1, Dimensions[rootsTE][[1]]}]  ]
     }, Alignment -> Center]
   , {\[Lambda], 0.3, 2.1, 0.03}];
ListAnimate[Reverse[modes], 2]

Licensing

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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

Modes allowed in an optical fibre as a function of wavelength.

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depicts

26 October 2020

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Date/TimeThumbnailDimensionsUserComment
current14:15, 28 October 2020Thumbnail for version as of 14:15, 28 October 2020600 × 386 (2.6 MB)BertoUploaded own work with UploadWizard
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