Chiral symmetry breaking and quark confinement in the nilpotency expansion of QCD

Sergio Caracciolo and Fabrizio Palumbo
Phys. Rev. D 83, 114504 – Published 2 June 2011

Abstract

We apply to lattice QCD a bosonization method previously developed in which dynamical bosons are generated by time-dependent Bogoliubov transformations. The transformed action can be studied by an expansion in the inverse of the nilpotency index, which is the number of fermionic states in the structure function of composite bosons. When this number diverges the model is solved by the saddle-point method which has a variational interpretation. We give a stationary covariant solution for a background matter field whose fluctuations describe mesons. In the saddle-point approximation fermionic quasiparticles exist which have quark quantum numbers. They are confined in the sense that they propagate only in pointlike color singlets. Conditions for chiral symmetry breaking are determined, to be studied numerically, and a derivation of a mesons-nucleons action is outlined.

  • Received 22 October 2010

DOI:https://doi.org/10.1103/PhysRevD.83.114504

© 2011 American Physical Society

Authors & Affiliations

Sergio Caracciolo*

  • Dipartimento di Fisica and INFN, Università degli Studi di Milano, via Celoria 16, I-20133 Milano, Italy

Fabrizio Palumbo

  • INFN–Laboratori Nazionali di Frascati, P.O. Box 13, I-00044 Frascati, Italy

  • *Sergio.Caracciolo@mi.infn.it
  • fabrizio.palumbo@lnf.infn.it

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Vol. 83, Iss. 11 — 1 June 2011

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