Non-Abelian gauge couplings at finite temperature and density

1988 ◽  
Vol 38 (10) ◽  
pp. 3211-3218 ◽  
Author(s):  
Hisao Nakkagawa ◽  
Hiroshi Yokota ◽  
Akira Niégawa
1988 ◽  
Vol 38 (8) ◽  
pp. 2566-2578 ◽  
Author(s):  
Hisao Nakkagawa ◽  
Akira Niégawa ◽  
Hiroshi Yokota

2011 ◽  
Vol 21 (3) ◽  
pp. 277
Author(s):  
Phan Hong Lien

The effective action and background field method have been applied to investigate free energy density for non-Abelian gauge theory at finite temperature, in which quantum corrections are included and certain symmetries of generating functional are restored. Renormalization is also considered for the gauge field. We give result for the one loop free energy density of gauge theory at high temperature and non-zero chemical potential, correcting a result previously at zero temperature and density. Some results are extended up to two loops


1992 ◽  
Vol 45 (4) ◽  
pp. 1432-1432 ◽  
Author(s):  
Naoki Ashida ◽  
Akira Niégawa ◽  
Hisao Nakkagawa ◽  
Hiroshi Yokota

2021 ◽  
Vol 2021 (10) ◽  
Author(s):  
D. S. Korneev ◽  
D. V. Plotnikov ◽  
K. V. Stepanyantz ◽  
N. A. Tereshina

Abstract We investigate the NSVZ relations for $$ \mathcal{N} $$ N = 1 supersymmetric gauge theories with multiple gauge couplings. As examples, we consider MSSM and the flipped SU(5) model, for which they easily reproduce the results for the two-loop β-functions. For $$ \mathcal{N} $$ N = 1 SQCD interacting with the Abelian gauge superfield we demonstrate that the NSVZ-like equation for the Adler D-function follows from the NSVZ relations. Also we derive all-loop equations describing how the NSVZ equations for theories with multiple gauge couplings change under finite renormalizations. They allow describing a continuous set of NSVZ schemes in which the exact NSVZ β-functions are valid for all gauge coupling constants. Very likely, this class includes the HD+MSL scheme, which is obtained if a theory is regularized by Higher covariant Derivatives and divergences are removed by Minimal Subtractions of Logarithms. That is why we also discuss how one can construct the higher derivative regularization for theories with multiple gauge couplings. Presumably, this regularization allows to derive the NSVZ equations for such theories in all loops. In this paper we make the first step of this derivation, namely, the NSVZ equations for theories with multiple gauge couplings are rewritten in a new form which relates the β-functions to the anomalous dimensions of the quantum gauge superfields, of the Faddeev-Popov ghosts, and of the matter superfields. The equivalence of this new form to the original NSVZ relations follows from the extension of the non-renormalization theorem for the triple gauge-ghost vertices, which is also derived in this paper.


2019 ◽  
Vol 34 (23) ◽  
pp. 1950128 ◽  
Author(s):  
A. F. Santos ◽  
Faqir C. Khanna

A non-Abelian gauge theory describes the strong interactions among particles with the commutator of generators are nonzero. An [Formula: see text] gauge theory describes the interactions that lead to nuclear forces among particles. The Lagrangian density refers to fermions with color and flavor and the gauge field quanta implying gluons. The gauge theory is treated at finite temperature using the Thermo Field Dynamics (TFD). Using self-interaction of gluons, the Stefan–Boltzmann law and the Casimir effect are calculated at finite temperature. An appendix is attached to give a response of a massless quarks in gauge theory.


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