Abstract
Quantum statistics will be discussed in the subsequent sections. One statement we will discuss beforehand. The most important and most widely used result is the following:
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Let us list the possible eigenvalues of a quantum mechanical system: E 1, ...,E 2 , ...,E j (V, N),.... Roughly speaking the E j ’s are the “possible energy values”; more exactly, they are defined by the Hamilton operator ℋ(V, N) of quantum theory which possesses eigenfunctions φ j,
$$H{\varphi _j} = {E_j}{\varphi _j}$$.
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© 1955 Springer-Verlag Berlin · Heidelberg
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Becker, R. (1955). Quantum Statistics. In: Theory of Heat. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-49255-6_3
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DOI: https://doi.org/10.1007/978-3-642-49255-6_3
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-642-49257-0
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