1981
DOI: 10.1016/0370-2693(81)90987-4
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Monte Carlo study of SU(2) gauge theory at finite temperature

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Cited by 431 publications
(150 citation statements)
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“…Using the well known value of Λ given by [12], we have Λ Λ critical (j = 1.00) = 1.226 ± 0.019 Λ Λ critical (j = 0.75) = 1.390 ± 0.025 Λ Λ critical (j = 0.50) = 1.572 ± 0.026 Λ Λ critical (j = 0.25) = 1.934 ± 0.031. (4.6) It is clear from these results that L critical z belongs to the confinement phase and there is a good agreement with the renormalization group equation (see Fig.…”
Section: The Presence Of the Unstable Mode On Latticementioning
confidence: 98%
“…Using the well known value of Λ given by [12], we have Λ Λ critical (j = 1.00) = 1.226 ± 0.019 Λ Λ critical (j = 0.75) = 1.390 ± 0.025 Λ Λ critical (j = 0.50) = 1.572 ± 0.026 Λ Λ critical (j = 0.25) = 1.934 ± 0.031. (4.6) It is clear from these results that L critical z belongs to the confinement phase and there is a good agreement with the renormalization group equation (see Fig.…”
Section: The Presence Of the Unstable Mode On Latticementioning
confidence: 98%
“…June 2001 Almost immediately after the ground-breaking demonstration that the numerical analysis of lattice regularized quantum field theories [1] can also provide quantitative results on fundamental non-perturbative properties of QCD [2] it has been realized that this approach will also allow to study the QCD phase transition [3,4] and the equation of state of the quark-gluon plasma [5]. During the last 20 years we have learned a lot from lattice calculations about the phase structure of QCD at finite temperature.…”
Section: Bi-tp 2001/10mentioning
confidence: 99%
“…The link variables Uµ(x) are elements of the SU (3) colour group. A product of these link variables around an elementary plaquette may be used to define an approximation to the gauge action, W (1,1) n,µν = 1 − 1 3 Re n,µν ≡ Re Tr Un,µU n+μ,ν U † n+ν,µ U † n,ν = g 2 a 4 2 F a µν F a µν + O(a 6 ) .…”
Section: Se(v T µ) ≡ Sg(v T ) + Sf (V T µ)mentioning
confidence: 99%
“…The thermodynamics of the phase transition at this temperature can be studied in two ways. On the one hand, one can evaluate the expectation value of a thermal Wilson loop [12,13], <lLi)=e r,/r/=0 T~<T~ (13)…”
Section: (L)mentioning
confidence: 99%
“…2, we present our results using Wilson's, Manton's and Villain's forms of the lattice action for SU(2) Yang-Mills theory. Besides T~ and o, we compare the deconfinement order parameter [12,13] (IL I) and the energy density ~ as functions of temperature for the different actions. In sect.…”
Section: Introductionmentioning
confidence: 99%