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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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书目名称Interacting Electrons and Quantum Magnetism
编辑Assa Auerbach
视频video
丛书名称Graduate Texts in Contemporary Physics
图书封面Titlebook: Interacting Electrons and Quantum Magnetism;  Assa Auerbach Textbook 1994 Springer Science+Business Media New York 1994 Boson.Hall effect.S
描述In the excitement and rapid pace of developments, writing pedagogical texts has low priority for most researchers. However, in transforming my lecture 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 colleagues; a kind of physics oral tradition passed between disciples of a similar faith. For many years, diagramatic perturbation theory has been the major theoretical tool for treating interactions in metals, semiconductors, itiner­ ant magnets, and superconductors. It is in essence a weak coupling expan­ sion about free quasiparticles. Many experimental discoveries during the last decade, including heavy fermions, fractional quantum Hall effect, high­ temperature superconductivity, and quantum spin chains, are not readily accessible from the weak coupling point of view. Therefore, recent years have seen vigorous development of alternative, nonperturbative tools for handling strong electron-electron interactions. I concentrate on two basic parad
出版日期Textbook 1994
关键词Boson; Hall effect; Superconductor; condensed matter; magnetism; spin exchange
版次1
doihttps://doi.org/10.1007/978-1-4612-0869-3
isbn_softcover978-1-4612-6928-1
isbn_ebook978-1-4612-0869-3Series ISSN 0938-037X
issn_series 0938-037X
copyrightSpringer Science+Business Media New York 1994
The information of publication is updating

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Nonlinear Sigma Model: Weak Couplingof freedom as the cubic zone (.) of the lattice . This determines the spherical Brillouin zone’s radius to be . Expanding the Hamiltonian in (13.2) in terms of gradients of . and keeping up to quadratic terms, the relation . is established at low temperatures (. << 1). The factor .. is the Boltzmann
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