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The most basic problem in quantum mechanics is to solve the stationary Schrodinger
equation for the energy eigenvalues and the associated energy eigenfunctions. There are
number of important cases for which the stationary Schrodinger equation can be solved
analytically. In most cases of practical interest exact or approximate numerical methods
must be employed. In this project solutions of Schrodinger equation in one-dimensional
problems are discussed. Numerov’s method which is very elegant fifth-order scheme
was derived and used. In dimensions higher than one, if the potential cannot be
separated, solving the Schrodinger equation numerically is, in general, quite a complex
problem. In practice, variational methods are therefore often used, where the wave
function is expanded in an incomplete set of conveniently chosen basis states. This
reduces the calculation to an eigenvalue problem in a discrete finite-dimensional space.
An example of variational calculation in square-well potential with an internal barrier is
shown. The matrix diagonalizations that have to be performed to solve the resulting
eigenvalue problem are discussed. |
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