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3d SU(N) + adjoint Higgs theory and finite temperature QCD
We study to what extent the three-dimensional SU(N)+adjoint Higgs theory can be used as an effective theory for finite temperature SU(N) gauge theory, with N=2,3. The parameters of the 3d theory are computed in 2-loop perturbation theory in terms of T/Lambda_MSbar,N,N_f. The perturbative effective p...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
1997
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/S0550-3213(97)00425-2 http://cds.cern.ch/record/324998 |
_version_ | 1780890888118992896 |
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author | Kajantie, K. Laine, M. Rummukainen, K. Shaposhnikov, Mikhail E. |
author_facet | Kajantie, K. Laine, M. Rummukainen, K. Shaposhnikov, Mikhail E. |
author_sort | Kajantie, K. |
collection | CERN |
description | We study to what extent the three-dimensional SU(N)+adjoint Higgs theory can be used as an effective theory for finite temperature SU(N) gauge theory, with N=2,3. The parameters of the 3d theory are computed in 2-loop perturbation theory in terms of T/Lambda_MSbar,N,N_f. The perturbative effective potential of the 3d theory is computed to two loops for N=2. While the Z(N) symmetry probably driving the 4d confinement-deconfinement phase transition (for N_f=0) is not explicit in the effective Lagrangian, it is partly reinstated by radiative effects in the 3d theory. Lattice simulations in the 3d theory are carried out for N=2, and the static screening masses relevant for the high-temperature phase of the 4d theory are measured. In particular, we measure non-perturbatively the O(g^2 T) correction to the Debye screening mass. We find that non-perturbative effects are much larger in the SU(2) + adjoint Higgs theory than in the SU(2) + fundamental Higgs theory. |
id | cern-324998 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1997 |
record_format | invenio |
spelling | cern-3249982022-07-06T02:23:23Zdoi:10.1016/S0550-3213(97)00425-2http://cds.cern.ch/record/324998engKajantie, K.Laine, M.Rummukainen, K.Shaposhnikov, Mikhail E.3d SU(N) + adjoint Higgs theory and finite temperature QCDParticle Physics - PhenomenologyWe study to what extent the three-dimensional SU(N)+adjoint Higgs theory can be used as an effective theory for finite temperature SU(N) gauge theory, with N=2,3. The parameters of the 3d theory are computed in 2-loop perturbation theory in terms of T/Lambda_MSbar,N,N_f. The perturbative effective potential of the 3d theory is computed to two loops for N=2. While the Z(N) symmetry probably driving the 4d confinement-deconfinement phase transition (for N_f=0) is not explicit in the effective Lagrangian, it is partly reinstated by radiative effects in the 3d theory. Lattice simulations in the 3d theory are carried out for N=2, and the static screening masses relevant for the high-temperature phase of the 4d theory are measured. In particular, we measure non-perturbatively the O(g^2 T) correction to the Debye screening mass. We find that non-perturbative effects are much larger in the SU(2) + adjoint Higgs theory than in the SU(2) + fundamental Higgs theory.We study to what extent the three-dimensional SU(N)+adjoint Higgs theory can be used as an effective theory for finite temperature SU(N) gauge theory, with N=2,3. The parameters of the 3d theory are computed in 2-loop perturbation theory in terms of T/Lambda_MSbar,N,N_f. The perturbative effective potential of the 3d theory is computed to two loops for N=2. While the Z(N) symmetry probably driving the 4d confinement-deconfinement phase transition (for N_f=0) is not explicit in the effective Lagrangian, it is partly reinstated by radiative effects in the 3d theory. Lattice simulations in the 3d theory are carried out for N=2, and the static screening masses relevant for the high-temperature phase of the 4d theory are measured. In particular, we measure non-perturbatively the O(g~2 T) correction to the Debye screening mass. We find that non-perturbative effects are much larger in the SU(2) + adjoint Higgs theory than in the SU(2) + fundamental Higgs theory.We study to what extent the three-dimensional SU(N)+adjoint Higgs theory can be used as an effective theory for finite temperature SU(N) gauge theory, with N=2,3. The parameters of the 3d theory are computed in 2-loop perturbation theory in terms of T/Lambda_MSbar,N,N_f. The perturbative effective potential of the 3d theory is computed to two loops for N=2. While the Z(N) symmetry probably driving the 4d confinement-deconfinement phase transition (for N_f=0) is not explicit in the effective Lagrangian, it is partly reinstated by radiative effects in the 3d theory. Lattice simulations in the 3d theory are carried out for N=2, and the static screening masses relevant for the high-temperature phase of the 4d theory are measured. In particular, we measure non-perturbatively the O(g~2 T) correction to the Debye screening mass. We find that non-perturbative effects are much larger in the SU(2) + adjoint Higgs theory than in the SU(2) + fundamental Higgs theory.We study to what extent the three-dimensional SU( N ) + adjoint Higgs theory can be used as an effective theory for finite-temperature SU( N ) gauge theory, with N = 2, 3. The parameters of the 3d theory are computed in 2-loop perturbation theory in terms of T/Λ MS , N and N f . The perturbative effective potential of the 3d theory is computed to two loops for N = 2. While the Z (N) symmetry probably driving the 4d confinement-deconfinement phase transition (for N f = 0) is not explicit in the effective Lagrangian, it is partly reinstated by radiative effects in the 3d theory. Lattice simulations in the 3d theory are carried out for N = 2, and the static screening masses relevant for the high-temperature phase of the 4d theory are measured. In particular, we measure non-perturbatively the O ( g 2 T ) correction to the Debye screening mass. We find that non-perturbative effects are much larger in the SU(2) + adjoint Higgs theory than in the SU(2) + fundamental Higgs theory.hep-ph/9704416CERN-TH-97-081CERN-TH-97-81BI-TP-97-10HD-THEP-97-17CERN-TH-97-081BI-TP-97-10HD-THEP-97-17oai:cds.cern.ch:3249981997-04-29 |
spellingShingle | Particle Physics - Phenomenology Kajantie, K. Laine, M. Rummukainen, K. Shaposhnikov, Mikhail E. 3d SU(N) + adjoint Higgs theory and finite temperature QCD |
title | 3d SU(N) + adjoint Higgs theory and finite temperature QCD |
title_full | 3d SU(N) + adjoint Higgs theory and finite temperature QCD |
title_fullStr | 3d SU(N) + adjoint Higgs theory and finite temperature QCD |
title_full_unstemmed | 3d SU(N) + adjoint Higgs theory and finite temperature QCD |
title_short | 3d SU(N) + adjoint Higgs theory and finite temperature QCD |
title_sort | 3d su(n) + adjoint higgs theory and finite temperature qcd |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/S0550-3213(97)00425-2 http://cds.cern.ch/record/324998 |
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