This Ising model was proposed in the 1924 doctoral thesis of Ernst Ising, a student of W. Lenz. Ising tried to explain
certain empirically observed facts about ferromagnetic materials using a model of proposed by
Lenz (1920). It was referred to in Heisenberg's (1928) paper which used the exchange mechanism to describe
ferromagnetism. The name became well-established with the publication of a paper by Peierls (1936), which gave a
non-rigorous proof that spontaneous magnetization must exist. A breakthrough occurred when it was shown that a
matrix
formulation of the model allows the partition function to be related to the largest
eigenvalue
of the matrix
(Kramers and Wannier 1941, Montroll 1941, 1942, Kubo 1943). Kramers and
Wannier (1941) calculated the Curie temperature using a two-dimensional Ising model, and a complete analytic solution was
subsequently given by Onsager (1944).
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