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Related papers: Bethe--Salpeter equation in QCD

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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 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

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

It is shown that the semirelativistic $q \bar{q}$ potential, the relativistic flux tube model and a confining Bethe--Salpeter equation can be derived from QCD first principles in a unified point of view.

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

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

Starting from a path integral representation of appropriate 4-point and 2-point gauge invariant Green functions and from the "Modified Area Law" model for the evaluation of the Wilson loop, a q \bar q Bethe-Salpeter like equation and a…

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

We briefly discuss the quark-antiquark Bethe-Salpeter equation and the quark Dyson-Schwinger equation derived in preceding papers. We also consider the q-qbar quadratic mass operator M^{2} = (w_{1} + w_{2})^{2} + U obtained by…

High Energy Physics - Phenomenology · Physics 2011-04-15 M. Baldicchi , G. M. Prosperi

We propose a novel method for the determination of the interquark potential together with quark "kinetic mass'' $m_Q$ from the equal-time $Q\bar{Q}$ Bethe-Salpeter (BS) amplitude in lattice QCD. Our approach allows us to calculate…

High Energy Physics - Lattice · Physics 2014-03-26 Taichi Kawanai , Shoichi Sasaki

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

We consider the solution of the Bethe-Salpeter equation in Euclidean metric for a qbar-q vector meson in the circumstance where the dressed quark propagators have time-like complex conjugate mass poles. This approximates features…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. Bhagwat , M. A. Pichowsky , P. C. Tandy

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

We investigate the Bethe--Salpeter description of mesons in the limit where one of the constituing quarks is infinitely heavy. To recover the non--relativistic quark model out of the Bethe--Salpeter formalism it is usual to assume that the…

High Energy Physics - Phenomenology · Physics 2010-11-01 A. Wambach

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 Bethe--Salpeter equations for the quark-antiquark composite systems with different quark masses, such as $q\bar s$ (with $q=u$,$d$), $q\bar Q$ and $s \bar Q$ (with $Q=c$,$b$), are written in terms of spectral integrals. For the mesons…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. V. Anisovich , V. V. Anisovich , V. N. Markov , M. A. Matveev , A. V. Sarantsev

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

We present an investigation of the interquark potential determined from the qq^bar Bethe-Salpeter (BS) amplitude for heavy quarkonia in lattice QCD. The qq^bar potential at finite quark mass m_q can be calculated from the equal-time and…

High Energy Physics - Lattice · Physics 2011-08-31 Taichi Kawanai , Shoichi Sasaki

Using the method of Green's functions within the framework of a Bethe-Salpeter formalism characterized by a pairwise $qq$ interaction with a 3D support to its kernel (expressed in a Lorentz-covariant manner), the 4D BS wave function for a…

High Energy Physics - Theory · Physics 2016-09-06 A. N. Mitra

A new method of solution of the Bethe-Salpeter equation for a pseudoscalar quark-antiquark bound state is proposed. With the help of an integral representation, the results are directly obtained in Minkowski space. Dressing of Green's…

High Energy Physics - Phenomenology · Physics 2014-11-18 V. Sauli

In the heavy quark limit, the heavy baryons \omega_{Q}^{(*)} (\omega could be \Sigma, \Xi or \Omega and Q=b or c) are regarded as composed of a heavy quark and an axial vector, light diquark with good spin and isospin quantum numbers. Based…

High Energy Physics - Phenomenology · Physics 2010-02-17 X. -H. Guo , A. W. Thomas , A. G. Williams
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