Quantum Gravitational Bremsstrahlung, Massless versus Massive Gravity

Simple item page
dc.creatorBerchtold, Julian B.
dc.creatorScharf, Gunter
dc.date2007-02-22
dc.date.accessioned2026-07-07T10:38:13Z
dc.date.available2026-07-07T10:38:13Z
dc.descriptionThe massive spin-2 quantum gauge theory previously developed is applied to calculate gravitational bremsstrahlung. It is shown that this theory is unique and free from defects. In particular, there is no strong coupling if the graviton mass becomes small. The cross sections go over smoothly into the ones of the massless theory in the limit of vanishing graviton mass. The massless cross sections are calculated for the full tensor theory.
dc.description13 pages, 1 figure
dc.identifierhttps://arxiv.org/abs/hep-th/0702181
dc.identifierhttp://arxiv.org/abs/hep-th/0702181
dc.identifierGen.Rel.Grav.39:1489-1502,2007
dc.identifierdoi:10.1007/s10714-007-0476-5
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/180646
dc.subjectHigh Energy Physics - Theory
dc.titleQuantum Gravitational Bremsstrahlung, Massless versus Massive Gravity
dc.typetext

Files

Collections

arXiv