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Phase Transition Couplings in the Higgsed Monopole Model

Using a one-loop approximation for the effective potential in the Higgs model of electrodynamics for a charged scalar field, we argue for the existence of a triple point for the renormalized (running) values of the selfinteraction beta-function as a typical quantity we estimate that the one-loop app...

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Autores principales: Laperashvili, L.V., Nielsen, Holger Bech
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:http://cds.cern.ch/record/401493
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author Laperashvili, L.V.
Nielsen, Holger Bech
author_facet Laperashvili, L.V.
Nielsen, Holger Bech
author_sort Laperashvili, L.V.
collection CERN
description Using a one-loop approximation for the effective potential in the Higgs model of electrodynamics for a charged scalar field, we argue for the existence of a triple point for the renormalized (running) values of the selfinteraction beta-function as a typical quantity we estimate that the one-loop approximation is valid with accuracy of deviations not more than 30% in the region of the parameters: $0.2 \stackrel{<}{\sim}{\large \alpha, \tilde{\alpha}} corresponds to the above-mentioned region of $\alpha, \tilde \alpha$. Under the point of view that the Higgs particle is a monopole with a magnetic charge g, the obtained electric fine structure constant turns out to be to the $\alpha_{crit}^{lat}\approx{0.20}$ which in a U(1) lattice gauge theory corresponds to the phase transition between the "Coulomb" and confinement phases. Such a result is very encouraging for the idea of an approximate "universality" (regularization independence) of gauge couplings at the phase transition point. This idea was suggested by the authors in their earlier papers.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1999
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spelling cern-4014932020-06-30T15:50:55Zhttp://cds.cern.ch/record/401493engLaperashvili, L.V.Nielsen, Holger BechPhase Transition Couplings in the Higgsed Monopole ModelParticle Physics - TheoryUsing a one-loop approximation for the effective potential in the Higgs model of electrodynamics for a charged scalar field, we argue for the existence of a triple point for the renormalized (running) values of the selfinteraction beta-function as a typical quantity we estimate that the one-loop approximation is valid with accuracy of deviations not more than 30% in the region of the parameters: $0.2 \stackrel{<}{\sim}{\large \alpha, \tilde{\alpha}} corresponds to the above-mentioned region of $\alpha, \tilde \alpha$. Under the point of view that the Higgs particle is a monopole with a magnetic charge g, the obtained electric fine structure constant turns out to be to the $\alpha_{crit}^{lat}\approx{0.20}$ which in a U(1) lattice gauge theory corresponds to the phase transition between the "Coulomb" and confinement phases. Such a result is very encouraging for the idea of an approximate "universality" (regularization independence) of gauge couplings at the phase transition point. This idea was suggested by the authors in their earlier papers.Using a one-loop approximation for the effective potential in the Higgs model of electrodynamics for a charged scalar field, we argue for the existence of a triple point for the renormalized (running) values of the selfinteraction $\lambda$ and the "charge" g given by $(\lambda_{run}, g^2) = (-{10/9} \pi^2,{4/3}\sqrt{{5/3}}{\pi^2}) \approx(-11, 17)$. Considering the beta-function as a typical quantity we estimate that the one-loop approximation is valid with accuracy of deviations not more than 30% in the region of the parameters: $0.2 \stackrel{<}{\sim}{\large \alpha, \tilde{\alpha}} \stackrel{<}{\sim}1.35.$ The phase diagram given in the present paper corresponds to the above-mentioned region of $\alpha, \tilde \alpha$. Under the point of view that the Higgs particle is a monopole with a magnetic charge g, the obtained electric fine structure constant turns out to be $\alpha_{crit}\approx{0.18_5}$ by the Dirac relation. This value is very close to the $\alpha_{crit}^{lat}\approx{0.20}$ which in a U(1) lattice gauge theory corresponds to the phase transition between the "Coulomb" and confinement phases. Such a result is very encouraging for the idea of an approximate "universality" (regularization independence) of gauge couplings at the phase transition point. This idea was suggested by the authors in their earlier papers.hep-th/9909181CERN-TH-99-275NBI-HE-99-1CERN-TH-99-275NBI-HE-99-1oai:cds.cern.ch:4014931999-09-27
spellingShingle Particle Physics - Theory
Laperashvili, L.V.
Nielsen, Holger Bech
Phase Transition Couplings in the Higgsed Monopole Model
title Phase Transition Couplings in the Higgsed Monopole Model
title_full Phase Transition Couplings in the Higgsed Monopole Model
title_fullStr Phase Transition Couplings in the Higgsed Monopole Model
title_full_unstemmed Phase Transition Couplings in the Higgsed Monopole Model
title_short Phase Transition Couplings in the Higgsed Monopole Model
title_sort phase transition couplings in the higgsed monopole model
topic Particle Physics - Theory
url http://cds.cern.ch/record/401493
work_keys_str_mv AT laperashvililv phasetransitioncouplingsinthehiggsedmonopolemodel
AT nielsenholgerbech phasetransitioncouplingsinthehiggsedmonopolemodel