scholarly journals Nf=2QCD chiral phase transition with Wilson fermions at zero and imaginary chemical potential

2016 ◽  
Vol 93 (11) ◽  
Author(s):  
Owe Philipsen ◽  
Christopher Pinke
Keyword(s):  
Phase Transition ◽  
Chemical Potential ◽  
Chiral Phase ◽  
Chiral Phase Transition ◽  
Wilson Fermions

scholarly journals Updates on the Columbia plot and its extended/alternative versions

2018 ◽  
Vol 175 ◽  
pp. 07032 ◽  
Author(s):  
Francesca Cuteri ◽  
Christopher Czaban ◽  
Owe Philipsen ◽  
Alessandro Sciarra
Keyword(s):  
Phase Transition ◽  
Critical Point ◽  
Continuum Limit ◽  
Chemical Potential ◽  
Chiral Phase ◽  
Chiral Phase Transition ◽  
Staggered Fermions ◽  
The Status ◽  
The Continuum ◽  
Wilson Fermions

We report on the status of ongoing investigations aiming at locating the deconfinement critical point with standard Wilson fermions and Nf = 2 flavors towards the continuum limit (standard Columbia plot); locating the tricritical masses at imaginary chemical potential with unimproved staggered fermions at Nf = 2 (extended Columbia plot); identifying the order of the chiral phase transition at μ = 0 for Nf = 2 via extrapolation from non integer Nf (alternative Columbia plot).

Studies on proper time regularization and the QCD chiral phase transition

2019 ◽  
Vol 34 (01) ◽  
pp. 1950003
Author(s):  
Yu-Qiang Cui ◽  
Zhong-Liang Pan
Keyword(s):  
Phase Transition ◽  
Small Parameter ◽  
Effective Mass ◽  
Finite Temperature ◽  
Chemical Potential ◽  
Proper Time ◽  
Chiral Phase ◽  
Chiral Phase Transition ◽  
Njl Model ◽  
The Difference

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.

scholarly journals Chiral phase transition in two-flavor QCD from an imaginary chemical potential

2014 ◽  
Vol 90 (7) ◽  
Author(s):  
Claudio Bonati ◽  
Philippe de Forcrand ◽  
Massimo D’Elia ◽  
Owe Philipsen ◽  
Francesco Sanfilippo
Keyword(s):  
Phase Transition ◽  
Chemical Potential ◽  
Chiral Phase ◽  
Chiral Phase Transition

Proper time regularization at finite quark chemical potential

2016 ◽  
Vol 31 (14) ◽  
pp. 1650086 ◽  
Author(s):  
Jin-Li Zhang ◽  
Yuan-Mei Shi ◽  
Shu-Sheng Xu ◽  
Hong-Shi Zong
Keyword(s):  
Phase Transition ◽  
Chemical Potential ◽  
Chiral Limit ◽  
Proper Time ◽  
Quark Confinement ◽  
Chiral Phase ◽  
Chiral Phase Transition ◽  
Njl Model ◽  
Potential Case ◽  
Chiral Susceptibility

In this paper, we use the two-flavor Nambu–Jona-Lasinio (NJL) model to study the quantum chromodynamics (QCD) chiral phase transition. To deal with the ultraviolet (UV) issue, we adopt the popular proper time regularization (PTR), which is commonly used not only for hadron physics but also for the studies with magnetic fields. This regularization scheme can introduce the infrared (IR) cutoff to include quark confinement. We generalize the PTR to zero temperature and finite chemical potential case use a completely new method, and then study the chiral susceptibility, both in the chiral limit case and with finite current quark mass. The chiral phase transition is second-order in [Formula: see text] and [Formula: see text] and crossover at [Formula: see text] and [Formula: see text]. Three sets of parameters are used to make sure that the results do not depend on the parameter choice.

The two-flavor NJL model with two-cutoff proper time regularization

2014 ◽  
Vol 29 ◽  
pp. 1460232 ◽  
Author(s):  
Zhu-Fang Cui ◽  
Yi-Lun Du ◽  
Hong-Shi Zong
Keyword(s):  
Phase Transition ◽  
Finite Temperature ◽  
Chemical Potential ◽  
Proper Time ◽  
Model Parameters ◽  
Chiral Phase ◽  
Chiral Phase Transition ◽  
Regularization Scheme ◽  
Njl Model

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.

scholarly journals Scaling properties of the chiral phase transition in the low density region of two-flavor QCD with improved Wilson fermions

2014 ◽  
Author(s):  
Takashi Umeda ◽  
Shinji Ejiri ◽  
Kazuyuki Kanaya ◽  
Yu Maezawa ◽  
Yoshiyuki Nakagawa ◽  
...  
Keyword(s):  
Phase Transition ◽  
Low Density ◽  
Density Region ◽  
Chiral Phase ◽  
Chiral Phase Transition ◽  
Scaling Properties ◽  
Wilson Fermions

scholarly journals The chiral phase transition of $N_f=2$ QCD at imaginary and zero chemical potential

2014 ◽  
Author(s):  
Owe Philipsen ◽  
Claudio Bonati ◽  
Massimo D'Elia ◽  
Philippe de Forcrand ◽  
Francesco Sanfilippo
Keyword(s):  
Phase Transition ◽  
Chemical Potential ◽  
Chiral Phase ◽  
Chiral Phase Transition
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