The QCD deconfinement transition for heavy quarks and all baryon chemical potentials

Journal of High Energy Physics

Volumn 2012, Issue 1, 2012, Pages

  Fromm, Michael ^a   Langelage, Jens ^a   Lottini, Stefano ^a   Philipsen, Owe ^a  

^a GOETHE UNIVERSITY   (Germany)

Author keywords

Heavy Quark Physics; Lattice QCD; Strong Coupling Expansion; Thermal Field Theory

Indexed keywords

EID: 84857281832     PISSN: 11266708     EISSN: 10298479     Source Type: Journal    
DOI: 10.1007/JHEP01(2012)042     Document Type: Article

References (33)

1. O. Philipsen, Lattice QCD at non-zero temperature and baryon density, arXiv:1009.4089 [INSPIRE].
2. K. Fukushima, Phase diagram from PNJL models, PoS(CPOD 2009)016 [INSPIRE].
3. W. Weise, Chiral symmetry in strongly interacting matter: from nuclear matter to phases of QCD, Prog. Theor. Phys. Suppl. 186 (2010) 390 [arXiv:1009.6201] [INSPIRE].
4. B.-J. Schaefer, Fluctuations and the QCDphase diagram, arXiv:1102.2772 [INSPIRE].
5. J. Luecker and C.S. Fischer, Two-flavor QCD at finite temperature and chemical potential in afunctional approach, arXiv:1111.0180 [INSPIRE].
6. L.M. Haas, J. Braun and J.M. Pawlowski, On the QCD phase diagram at finite chemical potential, AIP Conf. Proc. 1343 (2011) 459 [arXiv:1012.4735] [INSPIRE].
7. J. Langelage, S. Lottini and O. Philipsen, Centre symmetric 3d effective actions for thermal SU(N) Yang-Mills from strong coupling series, JHEP 02 (2011) 057 [Erratum ibid. 1107 (2011) 014] [arXiv:1010.0951] [INSPIRE].
8. R. De Pietri, A. Feo, E. Seiler and I.-O. Stamatescu, A modelfor QCD at high density and large quark mass, Phys. Rev. D 76 (2007) 114501 [arXiv:0705.3420] [INSPIRE].
9. I. Montvay and G. Münster, Quantum fields on a lattice, Cambridge monographs on mathematical physics, Cambridge University Press, Cambridge U.K. (1994).
10. f=0 heavy quark potential from short to intermediate distances, Nucl. Phys. B 622 (2002) 328 [hep-lat/0108008] [INSPIRE].
11. J. Langelage and O. Philipsen, The deconfinement transition offinite density QCD with heavy quarksfrom strong coupling series, JHEP 01 (2010) 089 [arXiv:0911.2577] [INSPIRE].
12. J. Langelage and O. Philipsen, The pressure ofstrong coupling lattice QCD with heavy quarks, the hadron resonance gas model and the large-N limit, JHEP 04 (2010) 055 [arXiv: 1002.1507] [INSPIRE] .
13. P. Hasenfratz and F. Karsch, Chemical potential on the lattice, Phys. Lett. B 125 (1983) 308 [INSPIRE].
14. M.G. Alford, S. Chandrasekharan, J. Cox and U. Wiese, Solution of the complex action problem in the Potts modelfor dense QCD, Nucl. Phys. B 602 (2001) 61 [hep-lat/0101012] [INSPIRE].
15. J. Condella and C.E. Detar, Potts flux tube model at nonzero chemical potential, Phys. Rev. D 61 (2000) 074023 [hep-lat/9910028] [INSPIRE].
16. C. Gattringer, Flux representation of an effective Polyakov loop model for QCD thermodynamics, Nucl. Phys. B 850 (2011) 242 [arXiv:1104.2503] [INSPIRE].
17. K. Eriksson, N. Svartholm and B. Skagerstam, On invariant group integrals in lattice QCD, J. Math. Phys. 22(1981) 2276 [INSPIRE].
18. J. Carlsson, Integrals overSU(N), arXiv:0802.3409 [INSPIRE].
19. N. Prokof'ev and B. Svistunov, Worm algorithms for classical statistical models, Phys. Rev. Lett. 87 (2001) 160601 [INSPIRE].
20. C. Gabriel, Dynamical properties of the worm algorithm, http://itp.tugraz.at/AG/AVP/thesis.html, Diploma thesis, Graz Austria (2002).
21. S. Kim, P. de Forcrand, S. Kratochvila and T. Takaishi, The 3-state Potts model as a heavy quarkfinite density laboratory, PoS(LAT2005)166 [hep-lat/0510069] [INSPIRE].
22. C. Alexandrou et al., The deconfinement phase transition in one flavor QCD, Phys. Rev. D 60 (1999) 034504 [hep-lat/9811028] [INSPIRE].
23. WHOT-QCD collaboration, H. Saito et al., Phase structure of finite temperature QCD in the heavy quark region, Phys. Rev. D 84 (2011) 054502 [arXiv:1106.0974] [INSPIRE].
24. Y. Deng and H.W. Bl̈ote, Simultaneous analysis of several models in the three-dimensional Ising universality class, Phys. Rev. E 68 (2003) 036125 [INSPIRE].
25. F. Green and F. Karsch, Mean field analysis ofSU(N) deconfining transitions in the presence of dynamical quarks, Nucl. Phys. B 238 (1984) 297 [INSPIRE].
26. N. Kawamoto and J. Smit, Effective Lagrangian and dynamical symmetry breaking in strongly coupled lattice QCD, Nucl. Phys. B 192 (1981) 100 [INSPIRE].
27. P. de Forcrand, S. Kim and O. Philipsen, A QCD chiral critical point at small chemical potential: is it there or not?, PoS(LATTICE 2007)178 [arXiv:0711.0262] [INSPIRE].
28. f = 2 + 1 QCD at zero and non-zero baryon density, JHEP 01 (2007) 077 [hep-lat/0607017] [INSPIRE].
29. 4, JHEP 11 (2008) 012 [arXiv:0808.1096] [INSPIRE].
30. P. de Forcrand and O. Philipsen, Constraining the QCD phase diagram by tricritical li nes at imaginary chemicalpotential, Phys. Rev. Lett. 105 (2010) 152001 [arXiv:1004.3144] [INSPIRE].
31. A. Roberge and N. Weiss, Gauge theories with imaginary chemical potential and the phases ofQCD, Nucl. Phys. B 275 (1986) 734 [INSPIRE].
32. C. Wozar, T. Kaestner, A. Wipf and T. Heinzl, Inverse Monte-Carlo determination of effective lattice models for SU(3) Yang-Mills theory at finite temperature, Phys. Rev. D 76 (2007) 085004 [arXiv:0704.2570] [INSPIRE].
33. P. de Forcrand, A. Kurkela and A. Vuorinen, Center-symmetric effective theory for high-temperature SU(2) Yang-Mills theory, Phys. Rev. D 77 (2008) 125014 [arXiv:0801.1566] [INSPIRE].