scholarly journals Critical region of the finite temperature chiral transition

1998 ◽  
Vol 58 (9) ◽  
Author(s):  
J. B. Kogut ◽  
M. A. Stephanov ◽  
C. G. Strouthos
1992 ◽  
Vol 280 (3-4) ◽  
pp. 261-266
Author(s):  
Nelson A. Alves ◽  
Bernd A. Berg ◽  
Dennis W. Duke ◽  
Anders Irbäck ◽  
Sergiu Sanielevici

2017 ◽  
Vol 45 ◽  
pp. 1760044 ◽  
Author(s):  
Ricardo L. S. Farias ◽  
Dyana C. Duarte ◽  
Gastão Krein ◽  
Rudnei O. Ramos

In this work we study the chiral transition in quark matter at finite temperature and in the presence of a chiral imbalance in the Nambu–Jona-Lasinio model. We use the Medium Separation Scheme (MSS) to rewrite divergent momentum integrals that appear in the model in such way that we can conciliate results obtained with the model and recent lattice results for the chiral transition.


2005 ◽  
Vol 2005 (02) ◽  
pp. 044-044 ◽  
Author(s):  
Francesco Basile ◽  
Andrea Pelissetto ◽  
Ettore Vicari

2007 ◽  
Vol 785 (1-2) ◽  
pp. 257-260 ◽  
Author(s):  
M. Kitazawa ◽  
T. Kunihiro ◽  
Y. Nemoto

1996 ◽  
Vol 10 (13n14) ◽  
pp. 1485-1497 ◽  
Author(s):  
M.A. VAN EIJCK ◽  
CH. G. VAN WEERT

We summarize results of the finite-temperature renormalization group approach, formalized by Matsumoto, Nakano and Umezawa in 1984, for the λ(ϕ4)4-model. The flow parameter is the reference temperature at which the mass parameter and the coupling constant of the theory are defined through renormalization conditions. We derive flow equations to one-loop order, and integrate numerically from zero temperature to above the critical temperature. The mass and the coupling constant both vanish at the critical temperature, and are positive below and above the critical region. In the critical region dimensional reduction to an effective 3D theory takes place. The leading behavior of the mass at high temperature is linear with a small logarithmic sub-leading contribution.


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