On the Fractional Parentage Expansions of Color Singlet Six Quark States in a Cluster Model
TL;DR: In this article, a color-singlet antisymmetric six-quark states in a cluster model with definite orbital and isospin-spin symmetries (symmetry basis) are given.
About: This article is published in Nuclear Physics.The article was published on 1981-02-09. It has received 192 citations till now. The article focuses on the topics: Isospin & Quark.
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1,525 citations
Abstract: We review how nuclear forces emerge from low-energy QCD via chiral effective field theory. The presentation is accessible to the non-specialist. At the same time, we also provide considerable detailed information (mostly in appendices) for the benefit of researchers who wish to start working in this field.
883 citations
TL;DR: In this article, the nuclear forces emerge from low-energy QCD via chiral eective theory, and the authors provide considerable detailed information for the benet of researchers who wish to start working in this field.
878 citations
TL;DR: In this article, the importance of light-cone dynamics, the physics of large longitudinal distances, and the presence of point-like quark-gluon configurations in hadrons for the theoretical description of high-energy processes (and especially nuclear shadowing) is explained.
446 citations
CERN1
TL;DR: In this paper, it has been realized that there must be corrections to this simple picture, for example, the meson exchange effects which preclude a simple interpretation of the magnetic moment of the deuteron in terms of d-state probability.
Abstract: Classical nuclear theory deals with a many-body system of neutrons and protons interacting nonrelativistically through two-body potentials. It has, of course, long been realized that there must be corrections to this simple picture—for example, the meson exchange effects which preclude a simple interpretation of the magnetic moment of the deuteron in terms of d-state probability. Nevertheless, the availability of beams of pions, and the consequent ability to study the excitation of real isobars in nuclei, has been critical in the realization that for many problems one must develop a theoretical model which explicitly includes pion and isobar degrees of freedom (see, for example, the proceedings of recent topical conferences Cat+ 82, MT 80).
428 citations
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TL;DR: In this paper, it was shown that a wide class of non-Abelian gauge theories have, up to calculable logarithmic corrections, free-field-theory asymptotic behavior.
Abstract: It is shown that a wide class of non-Abelian gauge theories have, up to calculable logarithmic corrections, free-field-theory asymptotic behavior. It is suggested that Bjorken scaling may be obtained from strong-interaction dynamics based on non-Abelian gauge symmetry.
3,334 citations
TL;DR: In the quark bag model, the same gluon-exchange forces which make the proton lighter than the $\ensuremath{\Delta}(1236)$ bind six quarks to form a stable, flavor-singlet (with strangeness of - 2) ${J}^{P}={0}^{+}$ dihyperon ($H$) at 2150 MeV as discussed by the authors.
Abstract: In the quark bag model, the same gluon-exchange forces which make the proton lighter than the $\ensuremath{\Delta}(1236)$ bind six quarks to form a stable, flavor-singlet (with strangeness of - 2) ${J}^{P}={0}^{+}$ dihyperon ($H$) at 2150 MeV. Another isosinglet dihyperon (${H}^{*}$) with ${J}^{P}={1}^{+}$ at 2335 MeV should appear as a bump in $\ensuremath{\Lambda}\ensuremath{\Lambda}$ invariant-mass plots. Production and decay systematics of the $H$ are discussed.
893 citations
702 citations
TL;DR: In this paper, a class of non-Abelian gauge theories of strong interactions is described, for which parity sand strangeness are automatically conserved, and for which the nonconservations of parity and strangeness produced by weak interactions are automatically of order alpha /m/sub w/sup 2/ rather than o f order alpha.
Abstract: ABS>A class of non-Abelian gauge theories of strong interactions is described, for which parity sand strangeness are automatically conserved, and for which the nonconservations of parity and strangeness produced by weak interactions are automatically of order alpha /m/sub w/sup 2/ rather than o f order alpha . When such theories are asymptotically free,'' the order- alpha weak corrections to natural zeroth-order symmetries may be calculated ignoring all effects of strong interactions. Speculations are offered on a possible theory of quarks. (auth)
450 citations
TL;DR: The hyperfine interaction between quarks suggested in chromodynamics can explain the size and pattern of the splittings and the mixing angles observed experimentally in nonstrange, negative parity baryons as discussed by the authors.
288 citations