Stochastic Quantization of Scalar Fields in Einstein and Rindler Spacetime
arXiv:0706.0920 · doi:10.1088/1751-8113/40/29/024
Abstract
We consider the stochastic quantization method for scalar fields defined in a curved manifold and also in a flat space-time with event horizon. The two-point function associated to a massive self-interacting scalar field is evaluated, up to the first order level in the coupling constant, for the case of an Einstein and also a Rindler Euclidean metric, respectively. Its value for the asymptotic limit of the Markov parameter is exhibited. The divergences therein are taken care of by employing a covariant stochastic regularization.
References in corpus (8)
- A Primer for Black Hole Quantum Physics
- Quantum Field Theory in Curved Spacetime
- Finite Size Effects in the Anisotropic λ/4!(ϕ^4_1 + ϕ^4_2)_d Model
- Effective Lagrangians for Scalar Fields and Finite Size Effects in Field Theory
- The Two-loop Massless phi^4 Model in Non-translational Invariant Domain
- Finite Size Effects in Thermal Field Theory
- Stochastic Quantization of Scalar Theory: Generalized Langevin Equation with Memory Kernel
- Stochastic Quantization of Topological Field Theory: Generalized Langevin Equation with Memory Kernel
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- Stochastic quantization of a self-interacting nonminimal scalar field in semiclassical gravity
- Stochastic Quantization of Real-Time Thermal Field Theory