Influence functional in two-dimensional dilaton gravity
We evaluate the influence functional for two-dimensional models of dilaton gravity. This functional is exactly computed when conformal invariance is preserved, and it can be written as the difference between the Liouville actions on each closed-time-path branch plus a boundary term. From the influen...
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1998
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paper:paper_05562821_v58_n2_p_Lombardo2023-06-08T15:42:21Z Influence functional in two-dimensional dilaton gravity Lombardo, Fernando César Mazzitelli, Francisco Diego We evaluate the influence functional for two-dimensional models of dilaton gravity. This functional is exactly computed when conformal invariance is preserved, and it can be written as the difference between the Liouville actions on each closed-time-path branch plus a boundary term. From the influence action we derive the covariant form of the semiclassical field equations. We also study the quantum to classical transition in cosmological backgrounds. In the conformal case we show that the semiclassical approximation is not valid because there is no imaginary part in the influence action. Finally we show that the inclusion of the dilaton loop in the influence functional breaks conformal invariance and ensures the validity of the semiclassical approximation. Fil:Lombardo, F.C. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Mazzitelli, F.D. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. 1998 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_05562821_v58_n2_p_Lombardo http://hdl.handle.net/20.500.12110/paper_05562821_v58_n2_p_Lombardo |
institution |
Universidad de Buenos Aires |
institution_str |
I-28 |
repository_str |
R-134 |
collection |
Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) |
description |
We evaluate the influence functional for two-dimensional models of dilaton gravity. This functional is exactly computed when conformal invariance is preserved, and it can be written as the difference between the Liouville actions on each closed-time-path branch plus a boundary term. From the influence action we derive the covariant form of the semiclassical field equations. We also study the quantum to classical transition in cosmological backgrounds. In the conformal case we show that the semiclassical approximation is not valid because there is no imaginary part in the influence action. Finally we show that the inclusion of the dilaton loop in the influence functional breaks conformal invariance and ensures the validity of the semiclassical approximation. |
author |
Lombardo, Fernando César Mazzitelli, Francisco Diego |
spellingShingle |
Lombardo, Fernando César Mazzitelli, Francisco Diego Influence functional in two-dimensional dilaton gravity |
author_facet |
Lombardo, Fernando César Mazzitelli, Francisco Diego |
author_sort |
Lombardo, Fernando César |
title |
Influence functional in two-dimensional dilaton gravity |
title_short |
Influence functional in two-dimensional dilaton gravity |
title_full |
Influence functional in two-dimensional dilaton gravity |
title_fullStr |
Influence functional in two-dimensional dilaton gravity |
title_full_unstemmed |
Influence functional in two-dimensional dilaton gravity |
title_sort |
influence functional in two-dimensional dilaton gravity |
publishDate |
1998 |
url |
https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_05562821_v58_n2_p_Lombardo http://hdl.handle.net/20.500.12110/paper_05562821_v58_n2_p_Lombardo |
work_keys_str_mv |
AT lombardofernandocesar influencefunctionalintwodimensionaldilatongravity AT mazzitellifranciscodiego influencefunctionalintwodimensionaldilatongravity |
_version_ |
1768544599811293184 |