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Related papers: Residual Gauge Fixing in Light-Front QCD

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The canonical quantization is performed at a light-front surface for the SU(N) Yang-Mills theory. The Weyl gauge is imposed as a gauge condition. The suitable parameterization is chosen for the transverse gauge field components in order to…

High Energy Physics - Theory · Physics 2007-05-23 Jerzy A. Przeszowski

We discuss the light-front zero-mode issue in the light-front quark model (LFQM) prediction of a vector meson decay constant from the perspective of the vacuum fluctuation consistent with the chiral symmetry of QCD. We extend the exactly…

High Energy Physics - Phenomenology · Physics 2015-06-17 Ho-Meoyng Choi , Chueng-Ryong Ji

We present a noncommutative gauge theory that has the ordinary Standard Model as its low-energy limit. The model is based on the gauge group U(4) x U(3) x U(2) and is constructed to satisfy the key requirements imposed by noncommutativity:…

High Energy Physics - Theory · Physics 2010-02-03 Valentin V. Khoze , Jonathan Levell

The light-front coupled-cluster (LFCC) method is a technique for solving Hamiltonian eigenvalue problems in light-front-quantized field theories. Its primary purpose is to provide a systematic sequence of solvable approximations to the…

High Energy Physics - Phenomenology · Physics 2013-10-03 S. S. Chabysheva , J. R. Hiller

We establish the ultra-violet finiteness of various classes of noncommutative gauge theories.

High Energy Physics - Theory · Physics 2009-11-07 I. Jack , D. R. T. Jones

Inspired by recent studies of high-scale decay constant or flavorful QCD axions, we review and clarify their existence in effective string models with anomalous $U(1)$ gauge groups. We find that such models, when coupled to charged scalars…

High Energy Physics - Phenomenology · Physics 2019-01-21 Quentin Bonnefoy , Emilian Dudas

In this paper we derive a gauge fixing identity by varying the covariant gauge fixing term in $Z[A,J,\eta, {\bar \eta}]$ in the background field method of QCD in pure gauge. Using this gauge fixing identity we establish a relation between…

High Energy Physics - Phenomenology · Physics 2010-08-17 Gouranga C Nayak

In this work we propose a way to promote the anomalous axial U(1) transformations to exact non-invertible U(1) symmetries. We discuss the procedure of coupling the non-invertible symmetry to a (dynamical or background) gauge field. We show…

High Energy Physics - Theory · Physics 2023-07-12 Avner Karasik

The breaking of chiral symmetry in holographic light-front QCD is encoded in its longitudinal dynamics with its chiral limit protected by the superconformal algebraic structure which governs its transverse dynamics. The scale in the…

High Energy Physics - Phenomenology · Physics 2022-01-05 Guy F. de Teramond , Stanley J. Brodsky

Gauge fields are special in the sense that they are invariant under gauge transformations and they lead to problems when we try quantizing them straightforwardly. To circumvent this problem we need to specify a gauge condition to fix gauge.

Nuclear Theory · Physics 2007-05-23 J. H. O. Sales

We have calculated the running coupling in SU(2), SU(3), and SU(4) gauge theories to see whether they have infrared fixed points. An infrared fixed point means no confinement: It means that the long-distance physics is conformal, without a…

High Energy Physics - Lattice · Physics 2013-01-10 Benjamin Svetitsky

We analyze the formation of fermionic condensates in two dimensional quantum chromodynamics for matter in the fundamental representation of the gauge group. We show that a topological regular instanton background is crucial in order to…

High Energy Physics - Theory · Physics 2009-10-31 Hugo Christiansen

We argue that gauge transformations with arbitrary fractional winding numbers should be allowed in a non-Abelian gauge theory. This eliminates the topological distinction between large and small gauge transformations. We prove that the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Valentin V. Khoze

The conformally invariant symmetric traceless field $A$ is considered. In four dimensions it possesses a scalar gauge invariance to which we provide a conformally invariant gauge fixing equation. A field strength $F$ is built upon $A$, its…

General Relativity and Quantum Cosmology · Physics 2025-12-08 Julien Queva

A new light-front formulation of Q.E.D. is developed, within the framework of standard perturbation theory, in which $x^+$ plays the role of the evolution parameter and the gauge choice is $A_+=0$ (light-front "temporal" gauge). It is shown…

High Energy Physics - Theory · Physics 2009-10-31 Michele Morara , Roberto Soldati

We investigate canonical structure of the Abelian Higgs model within the framework of DLCQ. Careful boundary analysis of differential equations, such as the Euler-Lagrange equations, leads us to a novel situation where the canonical…

High Energy Physics - Theory · Physics 2009-10-31 K. Itakura , S. Maedan , M. Tachibana

In principle, the complete spectrum and bound-state wave functions of a quantum field theory can be determined by finding the eigenvalues and eigensolutions of its light-cone Hamiltonian. One of the challenges in obtaining nonperturbative…

High Energy Physics - Phenomenology · Physics 2009-09-11 S. J. Brodsky , V. A. Franke , J. R. Hiller , G. McCartor , S. A. Paston , E. V. Prokhvatilov

Using the effective potential approach for composite operators we have formulated the quantum model of the QCD vacuum. It is based on the existence and importance of the nonperturbative $q^{-4}$-type dynamical, topologically nontrivial…

High Energy Physics - Phenomenology · Physics 2009-10-31 V. Gogohia , H. Toki , T. Sakai , Gy. Kluge

Numerical results for the (rest-frame) $Q\bar{Q}$ potential in light-front quantized $QCD_{2+1}$ on a $\perp$ lattice are presented. Both in the longitudinal as well as the $\perp$ spatial directions one obtains linear confinement. The…

High Energy Physics - Phenomenology · Physics 2007-05-23 Matthias Burkardt

We discuss invertible and non-invertible topological condensation defects arising from gauging a discrete higher-form symmetry on a higher codimensional manifold in spacetime, which we define as higher gauging. A $q$-form symmetry is called…

High Energy Physics - Theory · Physics 2023-11-02 Konstantinos Roumpedakis , Sahand Seifnashri , Shu-Heng Shao
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