Symmetry Breaking, Quark Deconfinement, and Deep-Inelastic Electron Scattering

It has recently been shown that deep-inelastic electron scattering from nuclei at large momentum transfer can be explained if quarks move in a larger effective volume in nuclei than in free nucleons. We argue that this ''partial deconfinement'' may be understood as arising from t...

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Veröffentlicht in:	Phys. Rev. Lett.; (United States) 1984-01, Vol.53 (9), p.892-894
Hauptverfasser:	Celenza, L. S., Rosenthal, A., Shakin, C. M.
Format:	Artikel
Sprache:	eng
Schlagworte:	645203 - High Energy Physics- Particle Interactions & Properties-Theoretical- Weak Interactions & Properties 645400 - High Energy Physics- Field Theory BOSON-EXCHANGE MODELS DEEP INELASTIC SCATTERING DIFFERENTIAL EQUATIONS ELECTRON-NUCLEON INTERACTIONS ELEMENTARY PARTICLES EQUATIONS EQUATIONS OF MOTION FIELD EQUATIONS FIELD THEORIES INELASTIC SCATTERING INTERACTIONS LEPTON-BARYON INTERACTIONS LEPTON-HADRON INTERACTIONS LEPTON-NUCLEON INTERACTIONS MATHEMATICAL MODELS MATTER MOMENTUM TRANSFER NUCLEAR MATTER OBE MODEL PARTIAL DIFFERENTIAL EQUATIONS PARTICLE INTERACTIONS PARTICLE MODELS PERIPHERAL MODELS PHYSICS OF ELEMENTARY PARTICLES AND FIELDS POSTULATED PARTICLES QUANTUM CHROMODYNAMICS QUANTUM FIELD THEORY QUARKS SCATTERING SYMMETRY BREAKING
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Zusammenfassung:	It has recently been shown that deep-inelastic electron scattering from nuclei at large momentum transfer can be explained if quarks move in a larger effective volume in nuclei than in free nucleons. We argue that this ''partial deconfinement'' may be understood as arising from the modification of symmetry-breaking dynamics as one passes from vacuum to nuclear matter.
ISSN:	0031-9007
DOI:	10.1103/PhysRevLett.53.892