IR finite correlation functions in de Sitter space, a smooth massless limit, and an autonomous equation
arXiv:2410.16226 · doi:10.1007/JHEP04(2025)127
Abstract
We explore two-point and four-point correlation functions of a massive scalar field on the flat de Sitter background in the long-wavelength approximation. By employing the Yang-Feldman-type equation, we compute the two-point correlation function up to order and the four-point correlation function up to order. In contrast to the standard theory of a massive scalar field based on the de Sitter-invariant vacuum, we develop a vacuum-independent reasoning that may not possess de Sitter invariance but results in a smooth massless limit of the correlation function's infrared part. Our elaboration allows us to calculate correlation functions of a free massive scalar field and to proceed with quantum corrections, relying only on the known infrared part of the two-point correlation function of a free massless one. Remarkably, the two-point correlation function of a free massive scalar field coincides with that of the Ornstein-Uhlenbeck stochastic process and has a clear physical interpretation. We compare our results with those obtained using the Schwinger-Keldysh diagrammatic technique, Starobinsky's stochastic approach, and the Hartree-Fock approximation. At last, we construct a renormalization group-inspired autonomous equation for the two-point correlation function. Integrating its approximate version, one obtains the non-analytic expression with respect to a self-interaction coupling constant . That solution reproduces the correct perturbative series up to the two-loop level. In the late-time limit, it almost coincides with the result of Starobinsky's stochastic approach over the whole interval of a new dimensionless parameter .
Equation (5.9) is corrected and corresponds to the upcoming erratum to the published version. All our subsequent conclusions remain unchanged. Some typos are corrected
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Cited by in corpus (4)
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- Scalar field stochastic dynamics in de Sitter spacetime from exact solutions of quantum deficient oscillators