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Related papers: Wilson loop approach to the qqbar interaction prob…

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We derive a confining $ q \bar{q}$ Bethe--Salpeter equation starting from the same assumptions on the Wilson loop integral already adopted in the derivation of a semirelativistic heavy quark potential. We show that, by standard…

High Energy Physics - Phenomenology · Physics 2016-11-03 N. Brambilla , G. M. Prosperi

We extend to regular QCD the derivation of a confining $ q \bar{q}$ Bethe--Salpeter equation previously given for the simplest model of scalar QCD in which quarks are treated as spinless particles. We start from the same assumptions on the…

High Energy Physics - Phenomenology · Physics 2014-11-17 N. Brambilla , E. Montaldi , G. M. Prosperi

The derivation of the $ q \bar q $ and the $ 3q $ potential for two dynamical quarks in a Wilson--loop context is reviewed. Some improvements are introduced. Only the usual assumptions in the evaluation of the Wilson loop integrals and…

High Energy Physics - Theory · Physics 2008-02-03 N. Brambilla , G. M. Prosperi

We review our recent results \cite{bsult} on the derivation of a B-S equation in QCD in a Wilson loop context. We work in a second order formalism, use the Feynman--Schwinger path integral representation for a quark in external field and…

High Energy Physics - Phenomenology · Physics 2007-05-23 N. Brambilla , G. M. Prosperi

Taking advantage of a semirelativistic and a full relativistic representation of the quark propagator in an external field we present an unified derivation of the semirelativistic potential and of a Bethe-Salpeter like equation for the…

High Energy Physics - Phenomenology · Physics 2016-09-06 N. Brambilla , G. M. Prosperi

The $Q \bar{Q}$ semirelativistic interaction in QCD can be simply expressed in terms of the Wilson loop and its functional derivatives. In this approach we present the $Q \bar{Q}$ potential up to order $1/m^2$ using the expressions for the…

High Energy Physics - Phenomenology · Physics 2009-10-28 N. Brambilla , A. Vairo

The $Q \bar{Q}$ semirelativistic interaction in QCD can be expressed in terms of the Wilson loop and its functional derivatives. In this framework we discuss the complete (velocity and spin dependent) $1/m^2$ potential in the stochastic…

High Energy Physics - Phenomenology · Physics 2007-05-23 N. Brambilla , A. Vairo

The complete $ q\bar{q}$ semirelativistic interaction is obtained as a gauge-invariant function of the Wilson loop and its functional derivatives. The approach is suitable for analytic evaluations as well as for lattice calculations. Here…

High Energy Physics - Phenomenology · Physics 2009-10-30 Nora Brambilla , Antonio Vairo

We give a nonperturbative derivation of the Bethe--Salpeter equation based on the Feynman--Schwinger path integral representation of the one--particle propagator in an external field. We apply the method to the quark--antiquark system in…

High Energy Physics - Phenomenology · Physics 2016-09-01 N. Brambilla , G. M. Prosperi

In lattice QCD, a confining potential for a static quark-antiquark pair can be computed with the Wilson loop technique. This potential, dominated by a linear potential at moderate distances, is consistent with the confinement with a flux…

High Energy Physics - Lattice · Physics 2011-07-14 P. Bicudo , G. Marques , M. Cardoso , N. Cardoso , O. Oliveira

First we review the derivation of the relativistic flux tube model for a quark-antiquark system from Wilson area law as we have given in a preceding paper. Then we extend the method to the three-quark case and obtain a Lagrangian…

High Energy Physics - Phenomenology · Physics 2016-09-01 N. Brambilla , G. M. Prosperi , A. Vairo

I revue the so called Wilson loop approach to bound state problem in QCD. I shall show how using appropriate path integral representations for the quark propagator in an external field it is possible to obtain corresponding path integral…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. M. Prosperi

Wilson loop averages are evaluated for large contours and in the large N limit by means of minimal surfaces. This allows the study of the quark-antiquark gauge invariant Green function through its dependence on Wilson loops. A covariant…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. Jugeau , H. Sazdjian

We calculate the static Wilson loop from string/gauge correspondence to obtain the $Q\bar Q$ potential in non-relativistic quantum field theory, i.e. CFT with Galilean symmetry. We analyze the convexity conditions \cite{bachas} for $Q\bar…

High Energy Physics - Theory · Physics 2015-05-28 Haryanto M. Siahaan

The quark-antiquark gauge invariant Green function is studied through its dependence on Wilson loops. The latter are saturated, in the large Nc limit and for large contours, by minimal surfaces. A covariant bound state equation is derived…

High Energy Physics - Phenomenology · Physics 2009-11-11 F. Jugeau , H. Sazdjian

In this paper we give a new derivation of the quark-antiquark potential in the Wilson loop context. This makes more explicit the approximations involved and enables an immediate extension to the three-quark case. In the $q\overline{q}$ case…

High Energy Physics - Theory · Physics 2009-10-28 N. Brambilla , P. Consoli , G. M. Prosperi

Bound q\bar q systems are studied in the framework of different 3-dimensional relativistic equations derived from the Bethe-Salpeter equation with the instantaneous kernel in the momentum space. Except the Salpeter equation, all these…

High Energy Physics - Phenomenology · Physics 2014-11-17 T. Babutsidze , T. Kopaleishvili , A. G. Rusetsky

Bound q\bar q -systems are considered in the framework of three different versions of the 3-dimensional reduction of the Bethe-Salpeter equation, all having the correct one-body limit when one of the constituent quark masses tends to…

High Energy Physics - Phenomenology · Physics 2009-10-30 T. Babutsidze , T. Kopaleishvili , A. Rusetsky

Within an effective field theory framework, we obtain an expression for the next-to-leading term in the $1/m$ expansion of the singlet $Q{\bar Q}$ QCD potential in terms of Wilson loops, which holds beyond perturbation theory. The…

High Energy Physics - Phenomenology · Physics 2014-12-23 N. Brambilla , A. Pineda , J. Soto , A. Vairo

An exactly soluble non-perturbative model of the pure gauge QCD is derived as a weak coupling limit of the lattice theory in plaquette formulation. The model represents QCD as a theory of the weakly interacting field strength fluxes. The…

High Energy Physics - Theory · Physics 2009-10-30 B. Rusakov
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