The deconfinement transition in SU(2) gauge theory: A finite-size analysis

S. Das; John B. Kogut

doi:10.1016/0550-3213(86)90311-1

The deconfinement transition in SU(2) gauge theory: A finite-size analysis

S. Das, John B. Kogut

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14 Scopus citations

Abstract

The finite-temperature deconfinement transition in pure SU(2) gauge theory is studied using finite-size analysis. The theory is formulated on a symmetric lattice with asymmetric couplings so the physical size of the spatial box can be changed continuously at a given physical temperature. Finite-size analysis based on the three-dimensional Ising model then permits the infinite-volume limit to be taken. The resulting critical temperature T_c scales according to asymptotic freedom and T_c/Λ_L = 44.0 ± 2.0.

Original language	English
Pages (from-to)	303-312
Number of pages	10
Journal	Nuclear Physics B
Volume	265
Issue number	2
DOIs	https://doi.org/10.1016/0550-3213(86)90311-1
State	Published - Feb 3 1986

Bibliographical note

Funding Information:
The computer simulations reported here were done on the CRAY-XMP/22 at NMFECC. We thank the DOE for support. The work of J.B.K. was partially supported by the National Science Foundation through the grant NSF PHY82-01948.

Funding

The computer simulations reported here were done on the CRAY-XMP/22 at NMFECC. We thank the DOE for support. The work of J.B.K. was partially supported by the National Science Foundation through the grant NSF PHY82-01948.

Funders	Funder number
National Science Foundation (NSF)	PHY82-01948

ASJC Scopus subject areas

Nuclear and High Energy Physics

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10.1016/0550-3213(86)90311-1

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title = "The deconfinement transition in SU(2) gauge theory: A finite-size analysis",

abstract = "The finite-temperature deconfinement transition in pure SU(2) gauge theory is studied using finite-size analysis. The theory is formulated on a symmetric lattice with asymmetric couplings so the physical size of the spatial box can be changed continuously at a given physical temperature. Finite-size analysis based on the three-dimensional Ising model then permits the infinite-volume limit to be taken. The resulting critical temperature Tc scales according to asymptotic freedom and Tc/ΛL = 44.0 ± 2.0.",

author = "S. Das and Kogut, \{John B.\}",

note = "Funding Information: The computer simulations reported here were done on the CRAY-XMP/22 at NMFECC. We thank the DOE for support. The work of J.B.K. was partially supported by the National Science Foundation through the grant NSF PHY82-01948.",

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AU - Kogut, John B.

N1 - Funding Information: The computer simulations reported here were done on the CRAY-XMP/22 at NMFECC. We thank the DOE for support. The work of J.B.K. was partially supported by the National Science Foundation through the grant NSF PHY82-01948.

PY - 1986/2/3

Y1 - 1986/2/3

N2 - The finite-temperature deconfinement transition in pure SU(2) gauge theory is studied using finite-size analysis. The theory is formulated on a symmetric lattice with asymmetric couplings so the physical size of the spatial box can be changed continuously at a given physical temperature. Finite-size analysis based on the three-dimensional Ising model then permits the infinite-volume limit to be taken. The resulting critical temperature Tc scales according to asymptotic freedom and Tc/ΛL = 44.0 ± 2.0.

AB - The finite-temperature deconfinement transition in pure SU(2) gauge theory is studied using finite-size analysis. The theory is formulated on a symmetric lattice with asymmetric couplings so the physical size of the spatial box can be changed continuously at a given physical temperature. Finite-size analysis based on the three-dimensional Ising model then permits the infinite-volume limit to be taken. The resulting critical temperature Tc scales according to asymptotic freedom and Tc/ΛL = 44.0 ± 2.0.

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JF - Nuclear Physics B

IS - 2

ER -

The deconfinement transition in SU(2) gauge theory: A finite-size analysis

Abstract

Bibliographical note

Funding

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