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Titlebook: Interacting Electrons and Quantum Magnetism; Assa Auerbach Textbook 1994 Springer Science+Business Media New York 1994 Boson.Hall effect.S

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樓主: Clique
31#
發(fā)表于 2025-3-26 21:13:32 | 只看該作者
32#
發(fā)表于 2025-3-27 01:50:17 | 只看該作者
Disorder in Low Dimensionsorder parameter does not eommute with the Hamiltonian. To foeus our diseussion, we eonsider a spin density wave in the z direetion defined by the operator . where i labels the lattiee sites and . is the ordering wave veetor.
33#
發(fā)表于 2025-3-27 06:55:45 | 只看該作者
From Ground States to Excitations of a good variational state—enables us to calculate the equal time spin correlations at . = 0. Experiments, however, can measure . at finite frequencies and at finite temperatures. It is clear from linear response theory (see Appendix B) that dynamical correlations depend on the . states and energies.
34#
發(fā)表于 2025-3-27 11:46:26 | 只看該作者
Quantum Antiferromagnets: Continuum Resultsns to those of the Nonlinear Sigma Model (NLSM) in .+1 dimensions with additional Berry phases. In Chapters 13 and 14, the correlation length ξ for the NLSM was found for .=1,2,3 using the continuum approximation.
35#
發(fā)表于 2025-3-27 13:44:53 | 只看該作者
The Continuum Approximation Mermin and Wagner’s Theorem 6.2, there can be no spontaneously broken symmetry at . > 0 in one and two dimensions. Moreover, we know that for the Heisenberg antiferromagnet in one dimension, we do not expect long-range spin order even at . = 0.
36#
發(fā)表于 2025-3-27 20:29:17 | 只看該作者
37#
發(fā)表于 2025-3-28 00:13:34 | 只看該作者
Textbook 1994 l notes into this book, I found a personal benefit: the organization of what I understand in a (hopefully simple) logical sequence. Very little in this text is my original contribution. Most of the knowledge was collected from the research literature. Some was acquired by conversations with colleag
38#
發(fā)表于 2025-3-28 04:23:55 | 只看該作者
39#
發(fā)表于 2025-3-28 09:51:55 | 只看該作者
40#
發(fā)表于 2025-3-28 12:16:46 | 只看該作者
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