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Collective electron ferromagnetism II. Energy and specific heat

Edmund Clifton Stoner

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Source: Crossref

Published: Feb 7, 1939

DOI: 10.1098/rspa.1939.0003

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Source abstract

Abstract A treatment of collective electron ferromagnetism on the basis of FermiDirac statistics was developed in a previous paper (Stoner 1938a, referred to as I). The problem considered was that of the magnetic characteristics associated with electrons in an energy band of standard form (in which the energy density of states is proportional to the square root of the energy), and subject to interchange interaction effects which involve dependence of the energy on the magnetization. The distribution of states is specified by a parameter e0, giving the maximum electron energy at absolute zero in the absence of the magnetization dependent part of the interchange interaction energy.

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