Talk:Eigenfunction Matching for a Finite Dock: Difference between revisions

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The link for the finite.m file is broken. Or maybe the file doesn't exist yet.
The link for the finite.m file is broken. Or maybe the file doesn't exist yet.
== Expression of the potential under the dock ==
It seems that the eigenfunctions
<math>
\frac{L\pm x}{2L}\psi_{0}(z)
</math>
do not satisfy the Laplace equation. Nor do any linear combination of them so it seems to me that we have to write <math>b_0=c_0=0</math> which means removing them from the potential expression.
Eigenfunctions <math>\frac{L\pm x}{2L}</math> work better but they will cause problems for infinite depth...

Revision as of 07:14, 12 April 2008

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