Chiral Quark Model of Nucleon Spin-Flavor Structure with SU(3) and Axial-U(1) Breakings
arXiv:hep-ph/9701248 · doi:10.1103/PhysRevD.57.344
Abstract
The chiral quark model with a nonet of Goldstone bosons can yield an adequate description of the observed proton flavor and spin structure. In a previous publication we have compared the results of a SU(3) symmetric calculation with the phenomenological findings based on experimental measurements and SU(3) symmetry relations. In this paper we discuss their SU(3) and axial-U(1) breaking corrections. With two parameters, we obtain a very satisfactory fit to the F/D ratios for the octet baryon masses and for their axial vector couplings, as well as the different quark flavor contributions to the proton spin. The result also can account for, not only the light u and d quark asymmetry, but also the strange quark content, of the proton sea. SU(3) breaking is the key in reconciling the strange quark fraction as measured in the neutrino charm production and that as deduced from the pion nuleon sigma term.
16 pages, Latex (uses Revtex), to be submitted to Phys. Rev. D
Cited by in corpus (42)
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- Magnetic Moments of Octet Baryons in Hot and Dense Nuclear Matter
- Magnetic moments of decuplet baryons using effective quark masses in chiral constituent quark model
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- Spin and Flavor Strange Quark Content of the Nucleon
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- Intrinsic strange distributions in the nucleon from the light-cone models
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- Polarized Structure of Nucleon in the Valon Representation
- Physics of the Nucleon Sea Quark Distributions
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- Chiral corrections to the vector and axial couplings of quarks and baryons
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- Strangeness and Chiral Symmetry Breaking
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- Electromagnetic and Axial-Vector Form Factors of the Quarks and Nucleon
- Phenomenological analysis of nucleon strangeness and meson-nucleon sigma terms
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- Study of the asymmetry in the proton
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