001     200818
005     20220628190223.0
024 7 _ |a 10.1103/PhysRevD.91.096002
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024 7 _ |a 0556-2821
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024 7 _ |a 1089-4918
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024 7 _ |a 1550-2368
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024 7 _ |a 1550-7998
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037 _ _ |a FZJ-2015-03203
082 _ _ |a 530
100 1 _ |a Francis, A.
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245 _ _ |a Critical point and scale setting in SU(3) plasma: An update
260 _ _ |a [S.l.]
|c 2015
|b Soc.
264 _ 1 |3 online
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|b American Physical Society (APS)
|c 2015-05-05
264 _ 1 |3 print
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|b American Physical Society (APS)
|c 2015-05-01
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520 _ _ |a We explore a method developed in statistical physics which has been argued to have exponentially small finite-volume effects, in order to determine the critical temperature ${T}_{\mathrm{c}}$ of pure SU(3) gauge theory close to the continuum limit. The method allows us to estimate the critical coupling ${\beta}_{c}$ of the Wilson action for temporal extents up to ${N}_{\tau}\sim20$ with $\lesssim0.1$% uncertainties. Making use of the scale setting parameters ${r}_{0}$ and $\sqrt{{t}_{0}}$ in the same range of $\beta$-values, these results lead to the independent continuum extrapolations ${T}_{\mathrm{c}}{r}_{0}=0.7457(45)$ and ${T}_{\mathrm{c}}\sqrt{{t}_{0}}=0.2489(14)$, with the latter originating from a more convincing fit. Inserting a conversion of ${r}_{0}$ from literature (unfortunately with much larger errors) yields ${T}_{\mathrm{c}}/{\mathrm{\Lambda}}_{\overline{\mathrm{MS}}}=1.24(10)$.
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536 _ _ |a Massive current--current correlators in thermal QCD (jara0108_20141101)
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|f Massive current--current correlators in thermal QCD
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536 _ _ |a Towards controlled QCD transport coefficients (jara0039_20121101)
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|f Towards controlled QCD transport coefficients
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542 _ _ |i 2015-05-05
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700 1 _ |a Kaczmarek, O.
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700 1 _ |a Laine, M.
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700 1 _ |a Neuhaus, T.
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700 1 _ |a Ohno, H.
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773 1 8 |a 10.1103/physrevd.91.096002
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|t Physical Review D
|v 91
|y 2015
|x 1550-7998
773 _ _ |a 10.1103/PhysRevD.91.096002
|g Vol. 91, no. 9, p. 096002
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|n 9
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