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Stochastic quantization

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This is an old revision of this page, as edited by Mark viking (talk | contribs) at 04:31, 8 March 2013 (Filled out the stub into a paragraph and added two references). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

In physics, stochastic quantization is a method for quantizing Euclidean field theories.[1] Stochastic quantization takes advantage of the fact that a Euclidean quantum field theory can be modeled as the equilibrium limit of a statistical mechanical system coupled to a heat bath. In particular, in the path integral representation of a Euclidean quantum field theory, the path integral measure is closely related to the Boltzmann distribution of a statistical mechanical system in equilibrium. In this relation, Euclidean Green's functions become correlation functions in the statistical mechanical system. A statistical mechanical system in equilibrium can be modeled, via the ergodic hypothesis, as the stationary distribution of a stochastic process. Then the Euclidean path integral measure can also be thought of as the stationary distribution of a stochastic process; hence the name stochastic quantization.

Stochastic quantization was introduced in 1981 by Parisi and Wu.[2] It is used for numerical applications such as numerical simulations of gauge theories with fermions. [1]

References

  1. ^ a b DAMGAARD, Poul (1987). "STOCHASTIC QUANTIZATION" (PDF). Physics Reports. 152 (5&6): 227–398. Retrieved 8 March 2013. {{cite journal}}: Unknown parameter |coauthors= ignored (|author= suggested) (help)
  2. ^ Parisi, G (1981). Sci. Sinica. 24: 483. {{cite journal}}: Missing or empty |title= (help); Unknown parameter |coauthors= ignored (|author= suggested) (help)