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C.1 The Infinite Potential Well

   The infinite potential well is a simple model for a  quantum dot (see Fig. C.1).
  
Figure C.1: The infinite potential well of width d.
\includegraphics{infinit_well.eps}

We are interested in the characteristic spacing between energy levels, especially the height of the first level. Starting with the Ansatz
\begin{alignat}{2}
\psi &= 0 &\qquad &x<0, x>d\\
\psi &= Ae^{\text{i}kx} + Be^{-\text{i}kx} &\qquad &0<x<d
\end{alignat}
and the boundary conditions
\begin{gather}\psi(0) = \psi(d) = 0
\end{gather}
non-trivial solutions are only possible for discrete wave vector values
\begin{gather}k=\frac{N\pi}{d}.
\end{gather}
And consequently the energy levels are
 \begin{gather}
E_N = \frac{\hbar^2k^2}{2m^*} = \frac{\hbar^2N^2\pi^2}{2m^*d^2} \qquad
N = 1, 2, \ldots
\end{gather}




Christoph Wasshuber