Delwedd:InfiniteSquareWellAnimation.gif
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InfiniteSquareWellAnimation.gif (300 × 280 picsel, maint y ffeil: 1,006 KB, ffurf MIME: image/gif, dolennog, 139 ffrâm, 14e)
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English: Trajectories of a particle in a box (also called an infinite square well) in classical mechanics (A) and quantum mechanics (B-F). In (A), the particle moves at constant velocity, bouncing back and forth. In (B-F), wavefunction solutions to the Time-Dependent Schrodinger Equation are shown for the same geometry and potential. The horizontal axis is position, the vertical axis is the real part (blue) or imaginary part (red) of the wavefunction. (B,C,D) are stationary states (energy eigenstates), which come from solutions to the Time-Independent Schrodinger Equation. (E,F) are non-stationary states, solutions to the Time-Dependent but not Time-Independent Schrodinger Equation. Both (E) and (F) are randomly-generated superpositions of the four lowest-energy eigenstates, (B-D) plus a fourth not shown. |
| Dyddiad | |
| Ffynhonnell | Gwaith fy hun |
| Awdur | Sbyrnes321 |
(*Source code written in Mathematica 6.0 by Steve Byrnes, Apr. 2011.
This source code is public domain.*)
(*Shows classical and quantum trajectory animations for an infinite-square-well potential.
Assumes L=hbar=1, m=2*pi^(-2), so that the nth energy eigenstate has energy n^2.*)
ClearAll["Global`*"]
(***Wavefunctions of the energy eigenstates***)
psi[n_, x_] := Sin[n*Pi*x]*2^(1/2);
energy[n_] := n^2;
psit[n_, x_, t_] := psi[n, x] Exp[-I*energy[n]*t];
(***A random time-dependent state***)
SeedRandom[1];
CoefList = Table[Random[]*Exp[2*Pi*I*Random[]], {n, 1, 4}];
CoefList = CoefList/Norm[CoefList];
Randpsi[x_, t_] := Sum[CoefList[[n]]*psit[n, x, t], {n, 1, 4}];
(***Another random time-dependent state***)
SeedRandom[2];
CoefList2 = Table[Random[]*Exp[2*Pi*I*Random[]], {n, 1, 3}];
CoefList2 = CoefList2/Norm[CoefList2];
Randpsi2[x_, t_] := Sum[CoefList2[[n]]*psit[n, x, t], {n, 1, 3}];
(***Set default style for plots***)
SetOptions[Plot,
{PlotRange -> {{-.05, 1.05}, {-2.5, 2.5}}, Ticks -> None,
PlotStyle -> {Directive[Thick, Blue], Directive[Thick, Pink]},
Axes -> {True, False}}];
SetOptions[ListPlot, {PlotRange -> {{-.05, 1.05}, {-2.5, 2.5}}, Axes -> False}];
(***Draw walls***)
walls = ListPlot[{{{0, -2.5}, {0, 2.5}}, {{1, -2.5}, {1, 2.5}}},
Joined -> True, PlotStyle -> {{Thick, Black}, {Thick, Black}}];
(***Make the classical plot...a red ball bounces back and forth.***)
classicaltrajectory[t_, left_, right_] := 2*(right - left)*Abs[t - Round[t]] + left;
classicalball[t_, left_, right_] := ListPlot[{{classicaltrajectory[t, left, right], 0}},
PlotStyle -> Directive[Red, AbsolutePointSize[15]]];
classical[t_, label_] := Show[walls, classicalball[t, .1, .9], PlotLabel -> label];
(***Make the quantum plots***)
plotpsi[n_, t_, label_] := Show[walls,
Plot[{Re[psit[n, x, t]], Im[psit[n, x, t]]}, {x, 0, 1}],
PlotLabel -> label, Axes -> {True, False}, Ticks -> None];
plotrand[t_, label_] := Show[walls,
Plot[{Re[Randpsi[x, t]], Im[Randpsi[x, t]]}, {x, 0, 1}],
PlotLabel -> label, Axes -> {True, False}, Ticks -> None];
plotrand2[t_, label_] := Show[walls,
Plot[{Re[Randpsi2[x, t]], Im[Randpsi2[x, t]]}, {x, 0, 1}],
PlotLabel -> label, Axes -> {True, False}, Ticks -> None];
(***Put all the plots together***)
MakeFrame[t_] := GraphicsGrid[
{{classical[3 t/(4 Pi), "A"], plotpsi[1, t, "B"]},
{plotpsi[2, t, "C"], plotpsi[3, t, "D"]},
{plotrand[t, "E"], plotrand2[t, "F"]}},
Frame -> All, ImageSize -> 300];
output = Table[MakeFrame[t], {t, 0, 4 Pi*138/139, 4 Pi/139}];
SetDirectory["C:\\Users\\Steve\\Desktop"]
Export["test.gif", output, "DisplayDurations" -> 10]
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| Dyddiad/Amser | Bawdlun | Hyd a lled | Defnyddiwr | Sylw | |
|---|---|---|---|---|---|
| cyfredol | 08:39, 27 Ebrill 2011 | | 300 × 280 (1,006 KB) | wikimediacommons>Sbyrnes321 | {{Information |Description ={{en|1=Trajectories of a particle in a box (also called an infinite square well) in classical mechanics (A) and quantum mechanics (B-F). In (A), the particle moves at constant velocity, bouncing back and forth. In (B-F), wav |
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