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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Main Authors: Laurent Baulieu, Siye Wu
Format: Article
Language:English
Published: Elsevier 2020-08-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321320301760
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spelling 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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