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23 - Functional integral approach to the theory of model Hamiltonians

Published online by Cambridge University Press:  01 June 2011

Victor Nikolaevich Popov
Affiliation:
Steklov Institute of Mathematics, St Petersburg
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Summary

In this section we outline the functional integral approach to the mathematically rigorous theory of the so-called model Hamiltonians system such as the Bardeen–Cooper–Schriffer (BCS) model in superconductivity (Bardeen, Cooper & Schriffer, 1957) or the Dicke model of superradiation. The problem of developing a rigorous theory of such models was put forward by Bogoliubov, Zubarev & Tserkovnikov (1960). This problem was solved for the BCS model by Bogoliubov (1960), who developed the so-called approximation Hamiltonian method. This method may be applied to the Dicke model as well. A rigorous theory of the Dicke model was suggested by Hepp & Lieb (1973). They have shown that there exists an exact solution of the model in the thermodynamic limit. The superradiation phase transition in this model was also described by these authors.

The approximation Hamiltonian method was applied to the Dicke model by Bogoliubov Jr (1974). Rigorous results for free energy and boson averages were obtained (see Bogoliubov Jr et al., 1981).

Functional integral methods were also applied to the Dicke model. Moshchinsky & Fedianin (1977) obtained asymptotics of Z/Z0, where Z is the partition function of the model and Z0 is the partition function of the corresponding free system. Kirianov and Yarunin (1980) investigated the Bose excitation spectrum of the system below the phase transition point in the superradiation state.

In this section we will prove the asymptotics of Z/Z0 for the Dicke model with a single mode of the radiation field (Popov & Fedotov, 1982).

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Publisher: Cambridge University Press
Print publication year: 1988

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