Abstract
In the early 1960’s one-dimensional model systems were regarded as amusing toys with the advantage of being far more easily solvable than their ’’real’’ three-dimensional counterparts. Now essentially 1-D (quasi-1-D) magnets can be ’’tailor-made’’ in the laboratory. Even more popular is the field of organic conductors like TTF⋅TCNQ, which are naturally quasi-1-D. Currently solitons and related solutions of non-linear, dispersive 1-D differential equations are ubiquitous in physics, including the area of 1-D magnetism. These developments are discussed in the Introduction. The rest of this paper is concerned with model Hamiltonians, model comparisons, critical singularities in 1-D (quasi-1-D) systems, accuracy of numerical techniques in comparison with exact solutions, brief accounts of dilute and disordered 1-D systems, and 1-D spin dynamics. Finally, a comment is made on a variety of interesting isomorphisms between 1-D magnets and phenomena in several other areas of physics, for example 2-D ferroelectrics, field-theoretic models, and realistic fluids. Comparison of theory and experiment has been the subject of several excellent reviews and is therefore not discussed here.
Highlights
Solitons and related solutions of non-linear, dispersive l-D differential equations are ubiquitous in physics, including the area of l-D magnetism
a comment is made on a variety of interesting isomorphisms between 1-D magnets and phenomena in 'several other areas of physics, for example 2-D ferroelectrics, fieldtheoretic models. and realistic fluids
The Ising model of cooperative magnetism was suggested by Lenz and solved in one-dimension (1-0) by Ising in 1925 [1]
Summary
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