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Naked singularities in dilatonic domain wall space-times

We investigate gravitational effects of extreme, non-extreme and ultra- extreme domain walls in the presence of a dilaton field. The dilaton is a scalar field without self-interaction that couples to the matter po- tential that is responsible for the formation of the wall. Motivated by superstring a...

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Detalles Bibliográficos
Autores principales: Cvetic, Mirjam, Soleng, Harald H.
Lenguaje:eng
Publicado: 1994
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.51.5768
http://cds.cern.ch/record/272572
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author Cvetic, Mirjam
Soleng, Harald H.
author_facet Cvetic, Mirjam
Soleng, Harald H.
author_sort Cvetic, Mirjam
collection CERN
description We investigate gravitational effects of extreme, non-extreme and ultra- extreme domain walls in the presence of a dilaton field. The dilaton is a scalar field without self-interaction that couples to the matter po- tential that is responsible for the formation of the wall. Motivated by superstring and supergravity theories, we consider both an exponential dilaton coupling (parametrized with the coupling constant alpha and the case where the coupling is self-dual, i.e. it has an extremum for a fi- nite value of the dilaton. For an exponential dilaton coupling, extreme walls (which are static planar configurations with surface energy density sigma_ext saturating the corresponding Bogomol'nyi bound) have a naked (planar) singularity outside the wall for alpha>1, while for alpha smaller or equal to 1 the singularity is null. On the other hand, non-extreme walls (bubbles with two insides and sigma_non > sigma_ext and ultra-extreme walls bubbles of false vacuum decay with sigma_ultra < sigma_ext always have naked singularities. There are solutions with self-dual couplings, which reduce to singularity-free vacuum domain wall space--times. However, only non- and ultra-extreme walls of such a type are dynamically stable.
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spelling cern-2725722020-07-23T02:49:14Zdoi:10.1103/PhysRevD.51.5768http://cds.cern.ch/record/272572engCvetic, MirjamSoleng, Harald H.Naked singularities in dilatonic domain wall space-timesParticle Physics - TheoryWe investigate gravitational effects of extreme, non-extreme and ultra- extreme domain walls in the presence of a dilaton field. The dilaton is a scalar field without self-interaction that couples to the matter po- tential that is responsible for the formation of the wall. Motivated by superstring and supergravity theories, we consider both an exponential dilaton coupling (parametrized with the coupling constant alpha and the case where the coupling is self-dual, i.e. it has an extremum for a fi- nite value of the dilaton. For an exponential dilaton coupling, extreme walls (which are static planar configurations with surface energy density sigma_ext saturating the corresponding Bogomol'nyi bound) have a naked (planar) singularity outside the wall for alpha>1, while for alpha smaller or equal to 1 the singularity is null. On the other hand, non-extreme walls (bubbles with two insides and sigma_non > sigma_ext and ultra-extreme walls bubbles of false vacuum decay with sigma_ultra < sigma_ext always have naked singularities. There are solutions with self-dual couplings, which reduce to singularity-free vacuum domain wall space--times. However, only non- and ultra-extreme walls of such a type are dynamically stable.We investigate gravitational effects of extreme, non-extreme and ultra- extreme domain walls in the presence of a dilaton field. The dilaton is a scalar field without self-interaction that couples to the matter po- tential that is responsible for the formation of the wall. Motivated by superstring and supergravity theories, we consider both an exponential dilaton coupling (parametrized with the coupling constant alpha and the case where the coupling is self-dual, i.e. it has an extremum for a fi- nite value of the dilaton. For an exponential dilaton coupling, extreme walls (which are static planar configurations with surface energy density sigma_ext saturating the corresponding Bogomol'nyi bound) have a naked (planar) singularity outside the wall for alpha>1, while for alpha smaller or equal to 1 the singularity is null. On the other hand, non-extreme walls (bubbles with two insides and sigma_non > sigma_ext and ultra-extreme walls bubbles of false vacuum decay with sigma_ultra < sigma_ext always have naked singularities. There are solutions with self-dual couplings, which reduce to singularity-free vacuum domain wall space--times. However, only non- and ultra-extreme walls of such a type are dynamically stable.hep-th/9411170UPR-0635-TCERN-TH-7475-94CERN-TH-7475-94UPR-635-Toai:cds.cern.ch:2725721994-11-23
spellingShingle Particle Physics - Theory
Cvetic, Mirjam
Soleng, Harald H.
Naked singularities in dilatonic domain wall space-times
title Naked singularities in dilatonic domain wall space-times
title_full Naked singularities in dilatonic domain wall space-times
title_fullStr Naked singularities in dilatonic domain wall space-times
title_full_unstemmed Naked singularities in dilatonic domain wall space-times
title_short Naked singularities in dilatonic domain wall space-times
title_sort naked singularities in dilatonic domain wall space-times
topic Particle Physics - Theory
url https://dx.doi.org/10.1103/PhysRevD.51.5768
http://cds.cern.ch/record/272572
work_keys_str_mv AT cveticmirjam nakedsingularitiesindilatonicdomainwallspacetimes
AT solengharaldh nakedsingularitiesindilatonicdomainwallspacetimes