Non‐local chiral quark model at finite chemical potential in the presence of an intense magnetic field

Author(s):  
Sebastián Alberto Ferraris ◽  
Ana Gabriela Grunfeld ◽  
Norberto Nerio Scoccola
1998 ◽  
Vol 437 (1-2) ◽  
pp. 24-28 ◽  
Author(s):  
Bojan Golli ◽  
Wojciech Broniowski ◽  
Georges Ripka

2006 ◽  
Vol 769 ◽  
pp. 35-52 ◽  
Author(s):  
Amir H. Rezaeian ◽  
Hans-Juergen Pirner

2009 ◽  
Vol 24 (11n13) ◽  
pp. 891-894
Author(s):  
SEUNG-IL NAM ◽  
HYUN-CHUL KIM

In this talk, we report our recent work on the pion weak decay constant (Fπ) and pion mass (mπ) using the nonlocal chiral quark model with the finite quark-number chemical potential (μ) taken into account. Considering the breakdown of Lorentz invariance at finite density, the time and space components are computed separately, and the corresponding results turn out to be: [Formula: see text] and [Formula: see text] at μc ≈ 320 MeV , respectively. Using the in-medium Gell-Mann-Oakes-Renner (GOR) relation, we show that the pion mass increases by about 15% at μc.


2010 ◽  
Vol 19 (08n10) ◽  
pp. 1703-1709 ◽  
Author(s):  
G. A. CONTRERA ◽  
M. ORSARIA ◽  
N. N. SCOCCOLA

We analyze the chiral restoration and deconfinement transitions in the framework of a non-local chiral quark model which includes terms leading to the quark wave function renormalization, and takes care of the effect of gauge interactions by coupling the quarks with the Polyakov loop. Non-local interactions are described by considering both a set of exponential form factors, and a set of form factors obtained from a fit to the mass and renormalization functions obtained in lattice calculations.


2021 ◽  
Vol 103 (7) ◽  
Author(s):  
Gang Yang ◽  
Jialun Ping ◽  
Jorge Segovia

Universe ◽  
2021 ◽  
Vol 7 (5) ◽  
pp. 155
Author(s):  
Xiaoyun Chen

In this work, the genuine resonance states of full-charm tetraquark systems with quantum numbers JPC=0++,1+−,2++ are searched in a nonrelativistic chiral quark model with the help of the Gaussian Expansion Method. In this calculation, two structures, meson-meson and diquark–antidiquark, as well as their mixing with all possible color-spin configurations, are considered. The results show that no bound states can be formed. However, resonances are possible because of the color structure. The genuine resonances are identified by the stabilization method (real scaling method). Several resonances for the full-charm system are proposed, and some of them are reasonable candidates for the full-charm states recently reported by LHCb.


2021 ◽  
Vol 103 (7) ◽  
Author(s):  
Oleksiy Roslyak ◽  
Godfrey Gumbs ◽  
Antonios Balassis ◽  
Heba Elsayed

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