scholarly journals Lattice QCD and High Baryon Density State

2011 ◽  
Author(s):  
Keitaro Nagata ◽  
Atsushi Nakamura ◽  
Shinji Motoki ◽  
Yoshiyuki Nakagawa ◽  
Takuya Saito ◽  
...  
2004 ◽  
Vol 129-130 ◽  
pp. 551-553
Author(s):  
Shin Muroya ◽  
Atsushi Nakamura ◽  
Chiho Nonaka

2004 ◽  
Vol 153 ◽  
pp. 51-59 ◽  
Author(s):  
Shin Muroya ◽  
Atsushi Nakamura ◽  
Chiho Nonaka

2014 ◽  
Vol 929 ◽  
pp. 157-168 ◽  
Author(s):  
M. Bluhm ◽  
P. Alba ◽  
W. Alberico ◽  
A. Beraudo ◽  
C. Ratti

2017 ◽  
Vol 45 ◽  
pp. 1760060 ◽  
Author(s):  
Ricardo L. S. Farias ◽  
Sidney S. Avancini ◽  
Marcus Benghi Pinto ◽  
William R. Tavares ◽  
Varese S. Timóteo

Within the framework of cold magnetized SU(2) Nambu-Jona-Lasinio model we evaluate the [Formula: see text] and [Formula: see text] pole mass, as well as, [Formula: see text], [Formula: see text] at zero baryon density. We employ a magnetic field dependent coupling, [Formula: see text], fitted to reproduce lattice QCD results for the quark condensates. In particular, we find that the [Formula: see text] meson mass systematically decreases when the magnetic field increases, in good agreement with recent lattice calculations.


2004 ◽  
Vol 30 (8) ◽  
pp. S1271-S1274 ◽  
Author(s):  
Krzysztof Redlich ◽  
Frithjof Karsch ◽  
Abdelnasser Tawfik

Author(s):  
SEYONG KIM

We briefly review recent progresses in studying QCD thermodynamics from lattice QCD. Investigation of QCD in zero baryon density shows a rapid cross-over with realistic (u, d, s) quark masses. Various improvements of lattice QCD action leads to more accurate determination of QCD thermodynamic properties. Although simulating QCD in non-zero baryon density is difficult due to "sign problem", steady progress is also achieved.


Author(s):  
V. G. Bornyakov ◽  
R. N. Rogalyov

Landau gauge longitudinal and transverse gluon propagators are studied in lattice QCD with gauge group [Formula: see text] at varying temperature and quark density. In particular, it is found that the longitudinal propagator decreases with increasing quark chemical potential at all temperatures under study, whereas the transverse propagator increases with increasing quark chemical potential at [Formula: see text] MeV and does not depend on it at higher temperatures. The relative strength of chromoelectric and chromomagnetic interactions is also discussed.


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