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In the world line representation of the fermionic effective action for QCD the interaction between Fermions and the gauge field is contained in the fermionic Wilson loop, namely the Wilson loop for a spin-half particle. It is argued that a…

High Energy Physics - Theory · Physics 2007-05-23 Vikram Vyas

We construct a classical vortex string solution in a Seiberg-dual theory of N=1 supersymmetric SO(N_c) QCD which flows to a confining phase. We claim that this vortex string is a QCD string, as previouly argued by M.Strassler. In SO(N_c)…

High Energy Physics - Theory · Physics 2009-04-30 Minoru Eto , Koji Hashimoto , Seiji Terashima

We present several clarifying comments on the loop pace self avoiding string representation for QCD(SU(infinity)) proposed by this author along last decade

General Physics · Physics 2019-09-04 Luiz C L Botelho

The confining string in presence of dynamical quarks can behave in different ways, depending on the quark masses and on the number N_f N_c of charge species. For light masses and large N_f N_c the creation of quark pairs produces…

High Energy Physics - Lattice · Physics 2015-06-25 F. Gliozzi , P. Provero

We calculate one loop corrections to the domain-wall quark propagator in QCD. We show how the wave function is renormalized in this theory. Especially we are interested in the behavior of the massless fermion mode, which exists near the…

High Energy Physics - Lattice · Physics 2009-10-30 S. Aoki , Y. Taniguchi

We discuss new results in QCD obtained with string-based methods. These methods were originally derived from superstring theory and are significantly more efficient than conventional Feynman rules. This technology was a key ingredient in…

High Energy Physics - Theory · Physics 2007-05-23 Z. Bern , L. Dixon , D. A. Kosower

We show how the gauge invariant formulation of QCD in terms of loops is free from a hidden $\theta$ parameter and offers an alternative way to solve the $U(1)_A$ puzzle.

High Energy Physics - Theory · Physics 2007-05-23 H. Fort , R. Gambini

We promote the usual QCD $\theta$-parameter to a field and interpret it as the phase of the quark condensate, which becomes nontrivial when topological defects, vortices in our formulation, are induced in the quark condensate by the QCD…

High Energy Physics - Phenomenology · Physics 2019-05-22 Chi Xiong

We describe a real-time classical solution of $c=1$ string field theory written in terms of the phase space density, $u(p,q,t)$, of the equivalent fermion theory. The solution corresponds to tunnelling of a single fermion above the filled…

High Energy Physics - Theory · Physics 2015-06-26 Avinash Dhar , Gautam Mandal , Spenta R. Wadia

String tension is introduced in perturbative QCD without hindering ultra violet renormalizability . The running gauge coupling constant remains unaltered and the string tension in the high energy limit vanishes asymptotically. Using 1/N…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ramesh Anishetty

In the standard model, stabilization of a classically unstable cosmic string may occur through the quantum fluctuations of a heavy fermion doublet. We review numerical results from a semiclassical expansion in a reduced version of the…

High Energy Physics - Theory · Physics 2015-08-12 H. Weigel , M. Quandt , N. Graham

The first observation is made of hadronic string breaking due to dynamical fermions in zero temperature lattice QCD. The simulations are done for SU(2) color in three dimensions, with two flavors of staggered fermions. The results have…

High Energy Physics - Lattice · Physics 2009-10-31 H. D. Trottier

I summarise what lattice methods can contribute to our understanding of the phenomenology of QCD at large Nc and describe some recent work on the physics of SU(Nc) gauge theories. These non-perturbative calculations show that there is…

High Energy Physics - Phenomenology · Physics 2017-08-23 M. Teper

A criterion to be satisfied by a string theory of QCD is formulated in the ultraviolet regime. It arises from the trace anomaly of the QCD stress tensor computed using instantons. It is sensitive to asymptotic freedom. It appears to be…

High Energy Physics - Theory · Physics 2009-12-30 B. S. Balakrishna

The equation for QCD string proposed earlier is reviewed. This equation appears when we examine the gonihedric string model and the corresponding transfer matrix. Arguing that string equation should have a generalized Dirac form we found…

High Energy Physics - Theory · Physics 2009-10-31 G. K. Savvidy

There are two cases where QCD string is described by an effective theory of long strings: the static potential and meson scattering amplitudes in the Regge regime. I show how the former can be solved in the mean-field approximation,…

High Energy Physics - Theory · Physics 2017-08-23 Yuri Makeenko

A new string theory is proposed as a candidate for the large N limit of QCD. In this theory, strings are constrained to be non-backtracking; a condition that is essential for the gauge invariance of the underlying field theory.This…

High Energy Physics - Theory · Physics 2009-10-22 Korkut Bardakci

We study the String dual to N=1 SQCD deformed by a quartic superpotential in the quark superfields. We present a unified view of the previous results in the literature and find new exact solutions and new asymptotic solutions. Then we study…

High Energy Physics - Theory · Physics 2008-11-26 Carlos Hoyos-Badajoz , Carlos Nunez , Ioannis Papadimitriou

We study the quantum dynamics of vortex strings in N=1 SQCD with U(N_c) gauge group and N_f=N_c quarks. The classical worldsheet of the string has N=(0,2) supersymmetry, but this is broken by quantum effects. We show how the pattern of…

High Energy Physics - Theory · Physics 2008-11-26 David Tong

Starting from the QCD Lagrangian we derive the effective action for massive quark and antiquark at large distances, corresponding to the minimal area low of the Wilson loop. The path integral method is used to quantize the system and the…

High Energy Physics - Phenomenology · Physics 2009-07-28 A. Yu. Dubin , A. B. Kaidalov , Yu. A. Simonov
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