Title: Some more waveforms
1 2The Time-dependent Schrödinger equation
Total energy Kinetic energy Potential
energy
The kinetic energy operator is
The potential energy operator is V
3Note that the left side is a function of time and
the right side is a function of position
time space
Therefore, I will assume any solution is a
product of a time-dependent portion and a space
dependent protion
4If I put this separated form into the TDSE
5And the separate them
The entire right side has no time-dependent
terms. So if I am solving for
6The entire right side has no time-dependent
terms. So if I am solving for
Where is just a constant
7I will rewrite this to get
I know that solutions to this are of the form
8It turns out that is related to the
energy, so I might as well write
Now I can write
9And when I put this back in the Time-dependent
Schrödinger equation
I get
This is the Time-independent Schrödinger equation
10Sometime it is more appropriate to write it as
Notice that now the energy looks more like an
independent variable that is part of the problem.
This is the case for the infinite well.
11If I were to rewrite this
with
It starts to look more like the type of wave
equations Im used to dealing with. If Egt V, I
will have positive values of k.
12Assuming one dimension
Solutions are of the form
or
i.e, propagating solutions
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21One the other hand, if EltV
then
22Which has solutions are of the form
i.e, decaying solutions
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32Note that the total energy remains the same!
33The following simulation is a pulse passing
through a slab of material. Notice that the
waveform changes wavelength as is goes through,
but then returns to its original form.
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44The following is similar, except EltV
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51What do you think will happen with the following
simulation?
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