Asymptotic Heat Kernels in Quantum Field Theory

dc.creatorEsposito, Giampiero
dc.date1995-06-23
dc.date.accessioned2026-07-07T03:30:42Z
dc.date.available2026-07-07T03:30:42Z
dc.descriptionAsymptotic expansions were first introduced by Henri Poincare in 1886. This paper describes their application to the semi-classical evaluation of amplitudes in quantum field theory with boundaries. By using zeta-function regularization, the conformal anomaly for a massless spin-${1\over 2}$ field in flat Euclidean backgrounds with boundary is obtained on imposing locally supersymmetric boundary conditions. The quantization program for gauge fields and gravitation in the presence of boundaries is then introduced by focusing on conformal anomalies for higher-spin fields. The conditions under which the covariant Schwinger-DeWitt and the non-covariant, mode-by-mode analysis of quantum amplitudes agree are described.
dc.description15 pages, plain-tex, appearing in Problems on High Energy Physics and Field Theory, Proceedings of the XVII Workshop, Dedicated to the 140th Anniversary of Henri Poincare, pp. 127-134 (Protvino: IHEP Pub. 1995)
dc.identifierhttps://arxiv.org/abs/gr-qc/9506048
dc.identifierhttp://arxiv.org/abs/gr-qc/9506048
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/35614
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleAsymptotic Heat Kernels in Quantum Field Theory
dc.typetext

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