Abstract
As explained in Part I, the stochastic limit technique does not apply only to the open system scheme, describing a discrete system interacting with a continuous one, but also to single continuous systems or to two (or more) mutually interacting continuous systems. The prototype of such systems is the Anderson model, proposed in [And58] to explain the finite conductivity of metals. It describes a system of fermions interacting with a classical Gaussian random field, modelling the impurities of the metal. If the classical field is discrete, we are in the framework described in Part I; even degree interaction bosonization takes place as described in Sect. 11.10.
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© 2002 Springer-Verlag Berlin Heidelberg
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Accardi, L., Volovich, I., Lu, Y.G. (2002). The Anderson Model. In: Quantum Theory and Its Stochastic Limit. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-04929-7_13
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DOI: https://doi.org/10.1007/978-3-662-04929-7_13
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-642-07543-8
Online ISBN: 978-3-662-04929-7
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