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10 - The Einstein–Langevin Equation

from Part III - Stochastic Gravity

Published online by Cambridge University Press:  20 January 2020

Bei-Lok B. Hu
Affiliation:
University of Maryland, College Park
Enric Verdaguer
Affiliation:
Universitat de Barcelona
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Summary

Whereas semiclassical gravity is based on the semiclassical Einstein equation with sources given by the expectation value of the stress-energy tensor, stochastic gravity is based on the Einstein–Langevin equation, which in addition has sources due to the noise kernel. The noise kernel is a bitensor which describes the quantum stress-energy tensor fluctuations of the matter fields. In this chapter we describe the fundamentals of this theory using an axiomatic and a functional approach. In the axiomatic approach, the equation is introduced as an extension of semiclassical gravity motivated by the search for self-consistent equations describing the backreaction of the stress-energy fluctuations on the gravitational field. We then discuss the equivalence between the stochastic correlation functions for the metric perturbations and the quantum correlation functions in the 1/N expansion, and illustrate the equivalence with a simple model. Based on the stochastic formulation, a criterion for the validity of semiclassical gravity is proposed. Alternatively, stochastic gravity is formulated using the Feynman–Vernon influence functional based on the open quantum system paradigm, in which the system of interest (the gravitational field) interacts with an environment (the matter fields).

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Chapter
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Semiclassical and Stochastic Gravity
Quantum Field Effects on Curved Spacetime
, pp. 337 - 363
Publisher: Cambridge University Press
Print publication year: 2020

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