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Self-consistent Quantum-Field Theory and Bosonization for Strongly Correlated Electron Systems

Author: Rudolf Haussmann
Publisher: Berlin, Heidelberg : Springer Berlin Heidelberg : Imprint: Springer, 1999.
Series: Lecture notes in physics., New series m,, Monographs ;, 56.
Edition/Format:   eBook : Document : English : 1st ed. 1999View all editions and formats
Summary:
This research monograph offers an introduction to advanced quantum field theoretical techniques for many-particle systems beyond perturbation theory. Several schemes for resummation of the Feynman diagrams are described. The resulting approximations are especially well suited for strongly correlated fermion and boson systems. Also considered is the crossover from BCS superconductivity to Bose--Einstein condensation  Read more...
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Genre/Form: Electronic books
Material Type: Document
Document Type: Book, Computer File
All Authors / Contributors: Rudolf Haussmann
ISBN: 3540489363 9783540489368
OCLC Number: 1167530290
Language Note: English.
Notes: Bibliographic Level Mode of Issuance: Monograph.
Description: 1 online resource (VIII, 175 p.).
Contents: Self-consistent quantum-field theory --
Superconductivity and pairing of electrons in three dimensions --
Gauge transformation and bosonization --
Two-dimensional electron systems in the FQHE regime --
Further applications.
Series Title: Lecture notes in physics., New series m,, Monographs ;, 56.
Responsibility: by Rudolf Haussmann.

Abstract:

This research monograph offers an introduction to advanced quantum field theoretical techniques for many-particle systems beyond perturbation theory. Several schemes for resummation of the Feynman diagrams are described. The resulting approximations are especially well suited for strongly correlated fermion and boson systems. Also considered is the crossover from BCS superconductivity to Bose--Einstein condensation in fermion systems with strong attractive interaction. In particular, a field theoretic formulation of "bosonization" is presented; it is published here for the first time. This method is applied to the fractional quantum Hall effect, to the Coulomb plasma, and to several exactly solvable models.

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