1998
DOI: 10.1103/physrevd.58.045001
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Chern-Simons number diffusion with hard thermal loops

Abstract: We construct an extension of the standard Kogut-Susskind lattice model for classical 3+1 dimensional Yang-Mills theory, in which "classical particle" degrees of freedom are added. We argue that this will correctly reproduce the "hard thermal loop" effects of hard degrees of freedom, while giving a local implementation which is numerically tractable. We prove that the extended system is Hamiltonian and has the same thermodynamics as dimensionally reduced hot Yang-Mills theory put on a lattice. We present a nume… Show more

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Cited by 118 publications
(158 citation statements)
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“…Moore, and others, have also obtained numerical results for the topological transition rate by using a more microscopic theory (analogous to a lattice version of what we called Theory 1) [31,32]. Moore also attempted to estimate the size of the NLLO correction to Γ by fitting the results of these simulations to the functional form…”
Section: Discussionmentioning
confidence: 99%
“…Moore, and others, have also obtained numerical results for the topological transition rate by using a more microscopic theory (analogous to a lattice version of what we called Theory 1) [31,32]. Moore also attempted to estimate the size of the NLLO correction to Γ by fitting the results of these simulations to the functional form…”
Section: Discussionmentioning
confidence: 99%
“…(See also Refs. [57,58] for a different lattice implementation of the HTL effects, and Refs. [79,80,81,82] for numerical calculations within purely Yang-Mills classical theory, without HTL's.…”
Section: Effective Theory For Soft and Ultrasoft Excitationsmentioning
confidence: 99%
“…This is relevant only for space-like (ω 2 < p 2 ) external momenta, since it is only for such momenta that the energy denominator ω −v · p can vanish. In that case, the polarization tensor (B.57) develops an imaginary part, 58) which describes the absorption or the emission of a space-like gluon, with four-momentum p µ = (ω, p), by a hard particle (quark or gluon) from the thermal bath (see, fig. 31 for an example).…”
Section: B12 the Ghost And Gluon Loopsmentioning
confidence: 99%
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