Equation of state in a strong magnetic field - Finite temperature and gradient corrections

1991 ◽  
Vol 374 ◽  
pp. 652 ◽  
Author(s):  
Andrew M. Abrahams ◽  
Stuart L. Shapiro
Keyword(s):  
Magnetic Field ◽  
Equation Of State ◽  
Strong Magnetic Field ◽  
Finite Temperature ◽  
Gradient Corrections

scholarly journals Equation of state of an anyon gas in a strong magnetic field

1994 ◽  
Vol 72 (5) ◽  
pp. 600-603 ◽  
Author(s):  
Alain Dasnières de Veigy ◽  
Stéphane Ouvry
Keyword(s):  
Magnetic Field ◽  
Equation Of State ◽  
Strong Magnetic Field

scholarly journals Effects of strong magnetic field on the formation of wakes in thermal QCD

2021 ◽  
Vol 36 (06) ◽  
pp. 2150045
Author(s):  
Mujeeb Hasan ◽  
Binoy Krishna Patra
Keyword(s):  
Magnetic Field ◽  
Charge Density ◽  
Strong Magnetic Field ◽  
Finite Temperature ◽  
Fast Moving ◽  
The Other ◽  
Other Hand ◽  
Induced Charge Density ◽  
Induced Charge ◽  
The Magnetic Field

We have investigated how the wakes in the induced charge density and in the potential due to the passage of highly energetic partons through a thermal QCD medium get affected by the presence of strong magnetic field [Formula: see text]. For that purpose, we wish to analyze first the dielectric responses of the medium both in presence and absence of strong magnetic field. Therefore, we have revisited the general form for the gluon self-energy tensor at finite temperature and finite magnetic field and then calculate the relevant structure functions at finite temperature and strong magnetic field limit (SMF: [Formula: see text] as well as [Formula: see text], [Formula: see text] is the electric charge (mass) of [Formula: see text]th flavor). We found that for slow moving partons, the real part of dielectric function is not affected by the magnetic field whereas for fast moving partons, for small [Formula: see text], it becomes very large and approaches towards its counterpart at [Formula: see text], for large [Formula: see text]. On the other hand the imaginary part is decreased for both slow and fast moving partons, due to the fact that the imaginary contribution due to quark loop vanishes. With these ingredients, we found that the oscillation in the (scaled) induced charge density, due to the very fast partons becomes less pronounced in the presence of strong magnetic field whereas for smaller parton velocity, no significant change is observed. For the (scaled) wake potential along the motion of fast moving partons (which is of Lennard–Jones (LJ-)type), the depth of negative minimum in the backward region gets reduced drastically, resulting in the reduction of the amplitude of oscillation. On the other hand in the forward region, it remains as the screened Coulomb one, except the screening now becomes much stronger for higher parton velocity. Similarly for the wake potential transverse to the motion of partons in both forward and backward regions, the depth of LJ potential for fast moving partons gets decreased severely, but still retains the forward–backward symm etry. However, for lower parton velocity, the magnetic field does not affect it significantly.

scholarly journals Induced charge and electric field in dense magnetized fermionic medium at finite temperature

2019 ◽  
Vol 27 (2) ◽  
pp. 9-16
Author(s):  
E. V. Reznikov ◽  
V. V. Skalozub
Keyword(s):  
Magnetic Field ◽  
Strong Magnetic Field ◽  
Finite Temperature ◽  
Chemical Potential ◽  
Potential Temperature ◽  
Integral Form ◽  
Dense Medium ◽  
Charge Dependence ◽  
Induced Charge ◽  
The One

The one-photon vertex in presence of strong magnetic field and finite temperature in dense medium is computed, its properties are investigated. Calculations are performed in analytical forms for two cases: at zero temperature and at high temperature. The integral form of the vertex is obtained for a general case. The tensor function is represented as the sum of Feynmanʼs one-loop diagrams. The induced charge dependence on chemical potential, temperature, and strong magnetic field is investigated in detail. The induced potential is calculated for the case of the infinite medium plate.

Sign in / Sign up

Export Citation Format

Share Document