Schwinger effect for non-Abelian gauge bosons
- 1. Institute of Experimental and Theoretical Physics Al-Farabi KazNU, Almaty, 050040 (Kazakhstan)
- 2. Department of Physics, California State University Fresno, Fresno, CA 93740-8031 (United States)
Description
We investigate the Schwinger effect for the gauge bosons in an unbroken non-Abelian gauge theory ( e.g. the gluons of QCD). We consider both constant "color electric" fields and "color magnetic" fields as backgrounds. As in the Abelian Schwinger effect we find there is production of "gluons" for the color electric field, but no particle production for the color magnetic field case. Since the non-Abelian gauge bosons are massless there is no exponential suppression of particle production due to the mass of the electron/positron that one finds in the Abelian Schwinger effect. Despite the lack of an exponential suppression of the gluon production rate due to the masslessness of the gluons, we find that the critical field strength is even larger in the non-Abelian case as compared to the Abelian case. This is the result of the confinement phenomenon on QCD. (paper)
Availability note (English)
Available from http://dx.doi.org/10.1088/1742-6596/883/1/012014Additional details
Identifiers
Publishing Information
- Journal Title
- Journal of Physics. Conference Series (Online)
- Journal Volume
- 883
- Journal Issue
- 1
- Journal Page Range
- [11 p.]
- ISSN
- 1742-6596
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 49065303
- Subject category
- S72: PHYSICS OF ELEMENTARY PARTICLES AND FIELDS;
- Descriptors DEI
- COMPARATIVE EVALUATIONS; CRITICAL FIELD; ELECTRIC FIELDS; ELECTRONS; GAUGE INVARIANCE; GLUONS; MASS; PARTICLE PRODUCTION; POSITRONS; QUANTUM CHROMODYNAMICS; SCHWINGER SOURCE THEORY
- Descriptors DEC
- ANTILEPTONS; ANTIMATTER; ANTIPARTICLES; BOSONS; ELEMENTARY PARTICLES; EVALUATION; FERMIONS; FIELD THEORIES; INVARIANCE PRINCIPLES; LEPTONS; MAGNETIC FIELDS; MATTER; QUANTUM FIELD THEORY