- #1
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- TL;DR Summary
- Approximating a finite potential step with a continuous function
Do any of you know of an article or book chapter that discusses the difference between a discontinuous potential well of length ##2L##
##V(x)=\left\{\begin{array}{cc}0, & |x-x_0 |<L\\V_0 & |x-x_0 |\geq L\end{array}\right.##
and a differentiable one
##\displaystyle V(x) = V_0 \exp\left[-\left(\frac{|x-x_0 |}{L}\right)^n\right]##
Edit: the correct equation above should have been
##\displaystyle V(x) = V_0 - V_0 \exp\left[-\left(\frac{|x-x_0 |}{L}\right)^n\right]##with ##n## some large but finite exponent (limit ##n\rightarrow\infty## is equivalent to the discontinuous version) ?
There was one article discussing the non-classical reflection of a wave packet at a downward potential step that considered the difference between these: https://aapt.scitation.org/doi/abs/10.1119/1.3636408
It should be possible to handle the difference between these two as a small perturbation, if the energy eigenstates and eigenvalues of the discontinuous basic potential well are already known (at least if ##V_0## isn't a very large or infinite number). Doing this for a 2D or 3D well of some shape would be more involved.
##V(x)=\left\{\begin{array}{cc}0, & |x-x_0 |<L\\V_0 & |x-x_0 |\geq L\end{array}\right.##
and a differentiable one
##\displaystyle V(x) = V_0 \exp\left[-\left(\frac{|x-x_0 |}{L}\right)^n\right]##
Edit: the correct equation above should have been
##\displaystyle V(x) = V_0 - V_0 \exp\left[-\left(\frac{|x-x_0 |}{L}\right)^n\right]##with ##n## some large but finite exponent (limit ##n\rightarrow\infty## is equivalent to the discontinuous version) ?
There was one article discussing the non-classical reflection of a wave packet at a downward potential step that considered the difference between these: https://aapt.scitation.org/doi/abs/10.1119/1.3636408
It should be possible to handle the difference between these two as a small perturbation, if the energy eigenstates and eigenvalues of the discontinuous basic potential well are already known (at least if ##V_0## isn't a very large or infinite number). Doing this for a 2D or 3D well of some shape would be more involved.
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