Delta Potential Born Approximation: Difference between revisions
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<math>f_B(\theta)=-\frac{m}{2\pi\hbar^2}\int V(r')e^{-i\mathbf{q}\cdot\mathbf{r}'}d^3r'</math> | <math>f_B(\theta)=-\frac{m}{2\pi\hbar^2}\int V(r')e^{-i\mathbf{q}\cdot\mathbf{r}'}d^3r'</math> | ||
where <math>mathbf{q}</math> | where <math>e^{-i\mathbf{q}\cdot\mathbf{r}'}</math> | ||
i\hbar\frac{\partial \psi(\textbf{r},t)}{\partial t} = \left[ -\frac{\hbar^2}{2m}\nabla^2 + V(\textbf{r})\right]\psi(\textbf{r},t | i\hbar\frac{\partial \psi(\textbf{r},t)}{\partial t} = \left[ -\frac{\hbar^2}{2m}\nabla^2 + V(\textbf{r})\right]\psi(\textbf{r},t |
Revision as of 21:27, 30 November 2009
Problem
Calculate the Born approximation to the differential and total cross sections for a particle of mass m off the -function potential .
Solution:
In Born approximation,
where
i\hbar\frac{\partial \psi(\textbf{r},t)}{\partial t} = \left[ -\frac{\hbar^2}{2m}\nabla^2 + V(\textbf{r})\right]\psi(\textbf{r},t