Weak and strong quantum vacuum: Properties of the different vacua
The ideas, definitions, and results of Castagnino and of Castagnino and Mazzitelli are improved and developed in a more general geometry. Also, a more satisfactory definition of the weak vacuum (defined by the coincidence of a local and a global property up to the lowest order) is introduced which y...
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1986
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paper:paper_05562821_v34_n12_p3676_Castagnino2023-06-08T15:42:03Z Weak and strong quantum vacuum: Properties of the different vacua Castagnino, Mario Alberto G. J. Chimento, Luis Pascual The ideas, definitions, and results of Castagnino and of Castagnino and Mazzitelli are improved and developed in a more general geometry. Also, a more satisfactory definition of the weak vacuum (defined by the coincidence of a local and a global property up to the lowest order) is introduced which yields a renormalization vacuum expectation value of the energy-momentum tensor. It is proved that a strong vacuum (defined by the same coincidence up to all orders) exists only in two particular cases: if there exists a Killing vector field or in the conformal massless case. © 1986 The American Physical Society. Fil:Castagnino, M.A. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Chimento, L. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. 1986 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_05562821_v34_n12_p3676_Castagnino http://hdl.handle.net/20.500.12110/paper_05562821_v34_n12_p3676_Castagnino |
institution |
Universidad de Buenos Aires |
institution_str |
I-28 |
repository_str |
R-134 |
collection |
Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) |
description |
The ideas, definitions, and results of Castagnino and of Castagnino and Mazzitelli are improved and developed in a more general geometry. Also, a more satisfactory definition of the weak vacuum (defined by the coincidence of a local and a global property up to the lowest order) is introduced which yields a renormalization vacuum expectation value of the energy-momentum tensor. It is proved that a strong vacuum (defined by the same coincidence up to all orders) exists only in two particular cases: if there exists a Killing vector field or in the conformal massless case. © 1986 The American Physical Society. |
author |
Castagnino, Mario Alberto G. J. Chimento, Luis Pascual |
spellingShingle |
Castagnino, Mario Alberto G. J. Chimento, Luis Pascual Weak and strong quantum vacuum: Properties of the different vacua |
author_facet |
Castagnino, Mario Alberto G. J. Chimento, Luis Pascual |
author_sort |
Castagnino, Mario Alberto G. J. |
title |
Weak and strong quantum vacuum: Properties of the different vacua |
title_short |
Weak and strong quantum vacuum: Properties of the different vacua |
title_full |
Weak and strong quantum vacuum: Properties of the different vacua |
title_fullStr |
Weak and strong quantum vacuum: Properties of the different vacua |
title_full_unstemmed |
Weak and strong quantum vacuum: Properties of the different vacua |
title_sort |
weak and strong quantum vacuum: properties of the different vacua |
publishDate |
1986 |
url |
https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_05562821_v34_n12_p3676_Castagnino http://hdl.handle.net/20.500.12110/paper_05562821_v34_n12_p3676_Castagnino |
work_keys_str_mv |
AT castagninomarioalbertogj weakandstrongquantumvacuumpropertiesofthedifferentvacua AT chimentoluispascual weakandstrongquantumvacuumpropertiesofthedifferentvacua |
_version_ |
1768542844340928512 |