Second order Langevin equation and definition of quantum gravity by stochastic quantisation
Euclidean quantum gravity might be defined by stochastic quantisation that is governed by a higher order Langevin equation rather than a first order stochastic equation. In a transitory phase where the Lorentz time cannot be defined, the parameter that orders the evolution of quantum gravity phenome...
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doaj-c6a1b9a160354a89acd4146b67daab392020-11-25T03:15:27ZengElsevierNuclear Physics B0550-32132020-08-01957115090Second order Langevin equation and definition of quantum gravity by stochastic quantisationLaurent Baulieu0Siye Wu1LPTHE, Sorbonne Université, CNRS, 4 Place Jussieu, 75005 Paris, France; Corresponding author.Department of Mathematics, National Tsing Hua University, 30013 Hsinchu, TaiwanEuclidean quantum gravity might be defined by stochastic quantisation that is governed by a higher order Langevin equation rather than a first order stochastic equation. In a transitory phase where the Lorentz time cannot be defined, the parameter that orders the evolution of quantum gravity phenomena is the stochastic time. This changes the definition of causality in the period of primordial cosmology. The prediction of stochastically quantised gravity is that there will a transition from an oscillating quantum phase to a semi-classical one, when the Lorentz time emerges. The end of the transition, as it can be observed from now and described by inflation models, is a diluted Universe, following the inflation phenomenological evolution. It is filled at the beginning with scattered classical primordial black holes. The smallest ones will quickly decay in matter, with a standard quantum field theory evolution till our period. The stable heavier black holes will remain, forming a good fraction of the dark matter and the large black holes observed in the galaxies. In a theoretically related way, this framework suggests the possibility of a gravitational parton content for “point-like” particles, in the same five dimensional quantum field theory context as in the primordial cosmology, with a (+−−−−) signature for the 5d metrics. The very precise and explicit result expressed in this paper is actually far more modest than its motivation. We compute explicitly the meaning of a second order Langevin equation in zero dimensions and define precisely what is second order stochastic quantisation in a soluble case.http://www.sciencedirect.com/science/article/pii/S0550321320301760 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Laurent Baulieu Siye Wu |
spellingShingle |
Laurent Baulieu Siye Wu Second order Langevin equation and definition of quantum gravity by stochastic quantisation Nuclear Physics B |
author_facet |
Laurent Baulieu Siye Wu |
author_sort |
Laurent Baulieu |
title |
Second order Langevin equation and definition of quantum gravity by stochastic quantisation |
title_short |
Second order Langevin equation and definition of quantum gravity by stochastic quantisation |
title_full |
Second order Langevin equation and definition of quantum gravity by stochastic quantisation |
title_fullStr |
Second order Langevin equation and definition of quantum gravity by stochastic quantisation |
title_full_unstemmed |
Second order Langevin equation and definition of quantum gravity by stochastic quantisation |
title_sort |
second order langevin equation and definition of quantum gravity by stochastic quantisation |
publisher |
Elsevier |
series |
Nuclear Physics B |
issn |
0550-3213 |
publishDate |
2020-08-01 |
description |
Euclidean quantum gravity might be defined by stochastic quantisation that is governed by a higher order Langevin equation rather than a first order stochastic equation. In a transitory phase where the Lorentz time cannot be defined, the parameter that orders the evolution of quantum gravity phenomena is the stochastic time. This changes the definition of causality in the period of primordial cosmology. The prediction of stochastically quantised gravity is that there will a transition from an oscillating quantum phase to a semi-classical one, when the Lorentz time emerges. The end of the transition, as it can be observed from now and described by inflation models, is a diluted Universe, following the inflation phenomenological evolution. It is filled at the beginning with scattered classical primordial black holes. The smallest ones will quickly decay in matter, with a standard quantum field theory evolution till our period. The stable heavier black holes will remain, forming a good fraction of the dark matter and the large black holes observed in the galaxies. In a theoretically related way, this framework suggests the possibility of a gravitational parton content for “point-like” particles, in the same five dimensional quantum field theory context as in the primordial cosmology, with a (+−−−−) signature for the 5d metrics. The very precise and explicit result expressed in this paper is actually far more modest than its motivation. We compute explicitly the meaning of a second order Langevin equation in zero dimensions and define precisely what is second order stochastic quantisation in a soluble case. |
url |
http://www.sciencedirect.com/science/article/pii/S0550321320301760 |
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