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This applet illustrates nonrelativistic quantum mechanical scattering from a square potential well of width L and finite energy depth V>0. The well is located between x=0 and x=L, and the incident wave approaches along the negative x axis.
The energy eigenstates are

where k and
are the wavenumbers outside and inside the
well, respectively. The eikx term is the incident wave, the R term is
the reflected wave, and the T term is the transmitted wave.
The unit of distance is chosen such that the state with k=0 has wavenumber
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inside the well.
The coefficients are given by

||2 is the reflection coefficient and ||2 is the transmission coefficient. (They satisfy ||2+||2=1.) The reflection coefficient is given by
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This has maxima at those values of k (the scattering resonances) for which
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The wavefunction whose probability distribution is animated by the applet has the form
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This is a finite sum of energy eigenstates weighted by a Gaussian centered at k0 with width proportional to Dk. The sum runs in equal steps from k0-Dk/2 to k0+Dk/2. A phase factor is included to center the incident wave packet around x=x0 at t=0. The unit of time is chosen such that the frequency is k2/2.
Notes:
| The location of the well is indicated by the red bar on the graph of the probability density. | |
| The momentum spectrum is superimposed in blue on the graph of the reflection coefficient. | |
| The incident wavepacket looks irregular because of interference with the reflected waves. |
Instructions for use
| Set the width L of the well (fixed at 30 in the demo) using the scrollbar provided. | |
| Set the initial position x0 of the incident wavepacket (fixed at -40 in the demo) using the scrollbar provided. | |
| Set the number of k values (fixed at 6 in the demo) using the popup menu. | |
| Set the central momentum k0 and width Dk using the scrollbars provided. | |
| Start, stop, resume, and reset using the buttons provided. | |
| After a run is stopped, any change in parameters resets the time to t=0. |
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