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Magnetic Component of Quark-Gluon Plasma is also a Liquid! · Around

2008

Magnetic Component of Quark-Gluon Plasma is also a Liquid!

Liao, Jinfeng, Shuryak, Edward

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The so called magnetic scenario recently suggested in \cite{Liao_ES_mono} emphasizes the role of monopoles in strongly coupled quark-gluon plasma (sQGP) near/above the deconfinement temperature, and specifically predicts that they help reduce its viscosity by the so called "magnetic bottle" effect.

Arguments for "magnetic liquid" in 1-2$T_c$ based on lattice measurement of monopole density were provided in \cite{Chernodub}.
Here we present results for monopole-(anti)monopole correlation functions from the same classical molecular dynamics simulations, which are found to be in very good agreement with recent lattice results \cite{D'Alessandro:2007su}.
We show that the magnetic Coulomb coupling does run in the direction $opposite$ to the electric one, as expected, and it is roughly inverse of the asymptotic freedom formula for the electric one.

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E. Shuryak, “QGP-new frontiers”, arXiv:0804.1373 [hep-ph]; “Physics of Strongly coupled Quark-Gluon Plasma,” arXiv:0807.3033 [hep-ph]
Original
Cited in the paper.
M. N. Chernodub and V. I. Zakharov, arXiv:0806.2874 [hep-ph]
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C. Ratti and E. Shuryak, in preparation
Cited in the paper.
Based on the monopole density they obtained on lattice, the authors of [ 2 ] suggested the magnetic component becomes gaseous above 2 T c T_{c} , see also separate argument in [ 17 ] . However the correlators from [ 3 ] clearly showed stronger correlation at higher T (see Fig. 2
Cited in the paper.

Then

B. A. Gelman, E. V. Shuryak and I. Zahed, Phys. Rev. C 74
2006
Later among the works it cites.
J. Liao and E. Shuryak, Phys. Rev. C 75
2007
Later among the works it cites.
M. N. Chernodub and V. I. Zakharov, Phys. Rev. Lett. 98
2007
Later among the works it cites.
A. D’Alessandro and M. D’Elia, Nucl. Phys. B 799
Original
2008
Closest in time.
J. Liao and E. Shuryak, Phys. Rev. C 77
2008
Closest in time.

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