Chiral phase transition inQED3at finite temperature and impurity potential

2016 ◽  
Vol 93 (1) ◽  
Author(s):  
Pei-Lin Yin ◽  
Wei Wei ◽  
Hai-Xiao Xiao ◽  
Hong-Tao Feng ◽  
Xiao-Jun Liu ◽  
...  
2019 ◽  
Vol 34 (01) ◽  
pp. 1950003
Author(s):  
Yu-Qiang Cui ◽  
Zhong-Liang Pan

We investigate the finite-temperature and zero quark chemical potential QCD chiral phase transition of strongly interacting matter within the two-flavor Nambu–Jona-Lasinio (NJL) model as well as the proper time regularization. We use two different regularization processes, as discussed in Refs. 36 and 37, separately, to discuss how the effective mass M varies with the temperature T. Based on the calculation, we find that the M of both regularization schemes decreases when T increases. However, for three different parameter sets, quite different behaviors will show up. The results obtained by the method in Ref. 36 are very close to each other, but those in Ref. 37 are getting farther and farther from each other. This means that although the method in Ref. 37 seems physically more reasonable, it loses the advantage in Ref. 36 of a small parameter dependence. In addition, we also, find that two regularization schemes provide similar results when T [Formula: see text] 100 MeV, while when T is larger than 100 MeV, the difference becomes obvious: the M calculated by the method in Ref. 36 decreases more rapidly than that in Ref. 37.


1994 ◽  
Vol 49 (12) ◽  
pp. 6822-6828 ◽  
Author(s):  
B. Rosenstein ◽  
A. D. Speliotopoulos ◽  
H. L. Yu

2009 ◽  
Vol 2009 (05) ◽  
pp. 035-035 ◽  
Author(s):  
Mohammad Edalati ◽  
Robert G Leigh ◽  
Nam Nguyen Hoang

Author(s):  
Zhu-Fang Cui ◽  
Yi-Lun Du ◽  
Hong-Shi Zong

In this paper, we use the two-flavor Nambu–Jona-Lasinio model together with the proper time regularization that has both ultraviolet and infrared cutoffs to study the chiral phase transition at finite temperature and zero chemical potential. The involved model parameters in our calculation are determined in the traditional way. Our calculations show that the dependence of the results on the choice of the parameters are really small, which can then be regarded as an advantage besides such a regularization scheme is Lorentz invariant.


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