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The Harmonic Oscillator

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Quantum Mechanics in Matrix Form
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Abstract

As a first application of the matrix method, the quantum mechanical behavior of the harmonic oscillator is discussed in detail.

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Notes

  1. 1.

    We assume that the restoring force f is proportional to the deflection; that is, \( f = -k x\).

  2. 2.

    Note that we get in fact

    $$\varvec{AA}^\dagger - \varvec{A}^\dagger \varvec{A} = \left( \begin{array}{cccc}1&{}0&{}0&{}\cdots \\ 0&{}2&{}0&{}\cdots \\ 0&{}0&{}3&{}\cdots \\ \vdots &{}\vdots &{}\vdots &{}\ddots \end{array}\right) - \left( \begin{array}{cccc}0&{}0&{}0&{}\cdots \\ 0&{}1&{}0&{}\cdots \\ 0&{}0&{}2&{}\cdots \\ \vdots &{}\vdots &{}\vdots &{}\ddots \end{array}\right) = \left( \begin{array}{cccc}1&{}0&{}0&{}\cdots \\ 0&{}1&{}0&{}\cdots \\ 0&{}0&{}1&{}\cdots \\ \vdots &{}\vdots &{}\vdots &{}\ddots \end{array}\right) = \varvec{I}.$$

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Correspondence to Günter Ludyk .

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Ludyk, G. (2018). The Harmonic Oscillator. In: Quantum Mechanics in Matrix Form. Springer, Cham. https://doi.org/10.1007/978-3-319-26366-3_5

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