By E. C. STONER,
Professor of Theoretical Physics, University of Leeds (England).
1. Introduction.
--- Although it has been suggested that participants in this conference should
survey generally the present position in the field
on which they are reporting, it would serve no
useful purpose for me to cover more hurriedly
precisely the same ground as do the recent comprehensive and general reviews of the theory of ferromagnetism by Van Vleck [1945, see also 1947, 1949]
and by myself [Stoner, 1948]. Further, one aspect
of the subject will be presented by Van Vleck
himself with far more authority than I could claim.
There are two main approaches to the theoretical
interpretation of the fundamental phenomena of
ferromagnetism, one deriving from the HeitlerLondon treatment of molecules, starting from atomic
wave functions, the other deriving from the electron energy band treatment of metals, which has a
close analogy with the Hund-Mulliken treatment of
molecules, using molecular orbitals. It is the second
approach with which I shall deal, and in particular
with the theoretical work at Leeds on what I have
ventured to call ((collective electron ferromagnetism».
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