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Kopsavilkums

Apraksts
English: Transfer matrix simulation of the dynamic of the electric field when a pulse is shone on a microcavity (in this case a Bragg reflector with a defect in the middle). Most of the pulse is reflected straight away, but the frequencies resonant with the cavity couple to it and the energy is stored in the confined mode. The cavity then relaxes exponentially with a time constant that depends on the Q-factor of the resonance.
Datums
Avots https://twitter.com/j_bertolotti/status/1075341329817853952
Autors Jacopo Bertolotti
Atļauja:
(Šī faila izmantošana citur)
https://twitter.com/j_bertolotti/status/1030470604418428929

Mathematica 11.0 code

c = 3 10^8; (*speed of light*)
M[n_, k_, d_] := {{Cos[n k d], I c/n Sin[n k d]}, {I n/c Sin[n k d], Cos[n k d]}}; (*transfer matrix*)
Mi[n_, k_, d_] := {{Cos[d k n], -((I c Sin[d k n])/n)}, {-((I n Sin[d k n])/c), Cos[d k n]}}; (*Inverse of a transfer matrix*)
t[m_, n0_, n2_] := (2 n0/c)/(n2/c m[[1, 1]] - (n0 n2)/c^2 m[[1, 2]] - m[[2, 1]] + n0/c m[[2, 2]]); (*transmission coefficient*)
d = 1 10^-6; (*layer thickness in m*)
dim = 6; (*number of layers in the Bragg mirror*)
s = Join[Table[1., 50], Table[If[EvenQ[j], 1., 2.], {j, 1, dim}], {1, 1}, Table[If[EvenQ[j], 1., 2.], {j, 1, dim}], Table[1., 50]] ;(*Reflective indices of each layer (including some space to show the pulse arrive*)
dim = Dimensions[s][[1]];
source = E^(-(1/2) (w - w0)^2 \[Sigma]^2) /. {w0 -> 2.185 10^15, \[Sigma] -> (10 10^-6)/c, a -> 10^12};
nstep = 2000;
\[Omega]min = 1.9 10^15;
\[Omega]max = 2.8 10^15;
sourcel = Table[source, {w, \[Omega]min, \[Omega]max, (\[Omega]max - \[Omega]min)/nstep}];
trasm = Reap[ For[\[Omega] = \[Omega]min, \[Omega] <= \[Omega]max, \[Omega] = \[Omega] + (\[Omega]max - \[Omega]min)/nstep,
tm = Apply[Dot, Table[M[s[[j]], \[Omega]/c, d], {j, 1, dim}]];
      Sow[N[t[tm, 1, 1]] ];
      ];][[2, 1]];
field = trasm*sourcel; (*Field at the last interface*)
sexpand = 5; (*increase spatial resolution*)
s2 = Flatten@Table[Table[s[[j]], sexpand], {j, 1, dim}];
freq = Table[j, {j, \[Omega]min, \[Omega]max, (\[Omega]max - \[Omega]min)/nstep}];
fn = Transpose[{field, field/c}];
tmp0 = fn;
ssm = Reap[For[i = dim*sexpand, i > 0, i--,
      tmp = Table[((Mi[s2[[i]], freq/c, d/sexpand])[[All, All, j]].tmp0[[j]]), {j, 1, nstep}];
      Sow[tmp[[All, 1]]];
      tmp0 = tmp;
      ];][[2, 1]];
fssm = Map[Fourier, ssm]; 
p1 = Table[
   ListPlot[{Re@Reverse@fssm[[All, -j]], Abs@Reverse@fssm[[All, -j]], -Abs@Reverse@fssm[[All, -j]]}, PlotRange -> {-7, 7}, Joined -> True, Axes -> False, PlotStyle -> {Directive[Orange], Directive[Thick, Black], Directive[Thick, Black]}, Epilog -> {Dashed, Black, Thick, Line[{{50*sexpand, -3}, {50*sexpand, 3}}], Line[{{64*sexpand, -3}, {64*sexpand, 3}}], Text[Style["Microcavity", Medium, Bold], 57*sexpand,         5}]} ], {j, -15, 200, 1}];
ListAnimate[Drop[p1, {16}], 10]

Licence

Es, šī darba autortiesību īpašnieks, publicēju to saskaņā ar šo licenci:
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.

This file, which was originally posted to https://twitter.com/j_bertolotti/status/1030470604418428929, was reviewed on 21 December 2018 by reviewer Ronhjones, who confirmed that it was available there under the stated license on that date.

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attēlo

19 decembris 2018

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