How hot are expanding universes ?

dc.creatorObadia, Nathaniel
dc.date2008-04-17
dc.date2008-10-16
dc.date.accessioned2026-07-07T11:49:57Z
dc.date.available2026-07-07T11:49:57Z
dc.descriptionA way to address the conundrum of Quantum Gravity is to illustrate the potentially fundamental interplay between quantum field theory, curved space-times physics and thermodynamics. So far, when studying moving quantum systems in the vacuum, the only known perfectly thermal temperatures are those obtained for constant (or null) accelerations $A$ in constant (or null) Hubble parameters $H$ space-times. In this Letter, restricting ourselves to conformally coupled scalar fields, we present the most comprehensive expression for the temperature undergone by a moving observer in the vacuum, valid for any time-dependent linear accelerations and Hubble parameters: $T=\sqrt{A^2 + H^2 + 2 \dot H\dot t}/{2π}$ where $\dot t=\d t/\d\t$ is the motion's Lorentz factor. The inequivalence between a constant $T$ and actual thermality is explained. As a byproduct, all the Friedman universes for which observers at rest feel the vacuum as a thermal bath are listed.
dc.description4 pages, no figure, version accepted in PRD
dc.identifierhttps://arxiv.org/abs/0804.2890
dc.identifierhttp://arxiv.org/abs/0804.2890
dc.identifierPhys.Rev.D78:083532,2008
dc.identifierdoi:10.1103/PhysRevD.78.083532
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/203419
dc.subjectGeneral Relativity and Quantum Cosmology
dc.subjectHigh Energy Physics - Theory
dc.titleHow hot are expanding universes ?
dc.typetext

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