Abstract
Many quantum spin systems of spin quantum number s > 1/2 or in spatial dimensions greater than 1D cannot be solved exactly. One source of this “lack of integrability” comes from the competition between different bonds, as in quantum frustration. We begin this final chapter by considering the application of approximate methods to one-dimensional models such as the spin-half J 1–J 2 model, and the spin-one Heisenberg and biquadratic models . The properties of the spin-half Heisenberg model for Archimedean lattices such as the square (unfrustrated) lattice, and the triangular and Kagomé (frustrated) lattices are listed for a variety of approximate techniques. The phenomenon of “order-from-disorder” is investigated in the context of the triangular lattice antiferromagnet in the presence of an external field. Finally, the properties of the square-lattice J 1–J 2 model and the Shastry-Sutherland model are studied. The chapter shows how the application of a range of approximate techniques, in addition to the few isolated exact results, can provide a comprehensive and compelling description of the ground-state properties of a wide range of quantum spin systems.
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Parkinson, J.B., Farnell, D.J. (2010). Quantum Magnetism. In: An Introduction to Quantum Spin Systems. Lecture Notes in Physics, vol 816. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-13290-2_11
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