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Revisiting strong coupling QCD at finite temperature and baryon density · Around

2008

Revisiting strong coupling QCD at finite temperature and baryon density

Fromm, M., de Forcrand, Ph.

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The strong coupling limit ($\beta_{gauge}=0$) of lattice QCD with staggered fermions enjoys the same non-perturbative properties as continuum QCD, namely confinement and chiral symmetry breaking.

In contrast to the situation at weak coupling, the sign problem which appears at finite density can be brought under control for a determination of the full (mu,T) phase diagram by Monte Carlo simulations.
Further difficulties with efficiency and ergodicity of the simulations, especially at the strongly first-order, low-T, finite-mu transition, are addressed respectively with a worm algorithm and multicanonical sampling.
Our simulations reveal sizeable corrections to the old results of Karsch and Muetter.

Built on

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Similar

G. Boyd, J. Fingberg, F. Karsch, L. Karkkainen and B. Petersson, Nucl. Phys. B 376
1992
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R. Aloisio et al., Nucl. Phys. B 564
2000
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N. Prokof’ev and B. Svistunov, Phys. Rev. Lett. 87
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D. H. Adams and S. Chandrasekharan, Nucl. Phys. B 662
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Y. Nishida, Phys. Rev. D 69
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K. Miura and A. Ohnishi, arXiv:0806.3357 [nucl-th]; N. Kawamoto, K. Miura and A. Ohnishi, arXiv:0710.1720 [hep-lat]; A. Ohnishi, N. Kawamoto and K. Miura, arXiv:0803.0255 [nucl-th]
Original
Cited in the paper.

Then

N. Kawamoto, K. Miura, A. Ohnishi and T. Ohnuma, Phys. Rev. D 75
2007
Later among the works it cites.
P. de Forcrand and S. Kim, Phys. Lett. B 645
2007
Later among the works it cites.
P. de Forcrand and O. Philipsen, JHEP 0701
Original
2007
Later among the works it cites.
F. Wang and D. P. Landau, Phys. Rev. Lett. 86
2050
Closest in time.

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