Chiral QCD, general QCD parametrization, and constituent quark models
Author:
Publisher
American Physical Society (APS)
Subject
Nuclear and High Energy Physics
Link
http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.68.014001/fulltext
Reference21 articles.
1. Effective field theory and the quark model. II. Structure of loop corrections
2. Erratum: Effective field theory and the quark model. II. Structure of loop corrections [Phys. Rev. D65, 034019 (2002)]
3. Effective field theory and the quark model
4. Field theory and the nonrelativistic quark model: A parametrization of the baryon magnetic moments and masses
5. Smallness of gluon coupling to constituent quarks in baryons and validity of nonrelativistic quark model
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2. $J^{P}=\frac{1}{2}^{+},\frac{3}{2}^{+}$ J P = 1 2 + , 3 2 + masses in the statistical model;The European Physical Journal A;2016-11
3. Magnetic moment for the negative parity Λ → Σ 0 transition in light cone QCD sum rules;Physics Letters B;2016-07
4. CHARGE RADII OF SPIN $\frac{1}{2}^+$ AND SPIN $\frac{3}{2}^+$ CHARMED BARYONS IN THE CHIRAL CONSTITUENT QUARK MODEL;International Journal of Modern Physics A;2013-05-30
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