2000
DOI: 10.1103/physrevd.62.014025
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Mesonlike baryons and the spin-orbit puzzle

Abstract: I describe a special class of meson-like Λ Q excited states and present evidence supporting the similarity of their spin-independent spectra to those of mesons. I then examine spin-dependent forces in these baryons, showing that predicted effects of spin-orbit forces are small for them for the same reason they are small for the analogous mesons: a fortuitous cancellation between large spin-orbit forces due to one-gluon-exchange and equally large inverted spin-orbit forces due to Thomas precession in the confin… Show more

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Cited by 72 publications
(107 citation statements)
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“…This favors a linear form for confinement as also suggested by meson spectroscopy and lattice calculations [160]. We should finally say that the level ordering problem has been cured by means of appropriate phenomenological interactions as has been the case of anharmonic terms [161], scalar three-body forces [162] or pseudoscalar interactions [45,163], but without any connection to a consistent simultaneous description of the baryon-baryon interaction except for reference [163]. [164], applicable only for the ground state of the system, assumes that the ground state three-particle wave function depends on a single variable R = 1 2 (x 1 + x 2 + ηx 3 ), where x i = | r j − r k | with r j,k the particle coordinates and ǫ ijk = 1.…”
Section: The Baryon Spectrummentioning
confidence: 99%
“…This favors a linear form for confinement as also suggested by meson spectroscopy and lattice calculations [160]. We should finally say that the level ordering problem has been cured by means of appropriate phenomenological interactions as has been the case of anharmonic terms [161], scalar three-body forces [162] or pseudoscalar interactions [45,163], but without any connection to a consistent simultaneous description of the baryon-baryon interaction except for reference [163]. [164], applicable only for the ground state of the system, assumes that the ground state three-particle wave function depends on a single variable R = 1 2 (x 1 + x 2 + ηx 3 ), where x i = | r j − r k | with r j,k the particle coordinates and ǫ ijk = 1.…”
Section: The Baryon Spectrummentioning
confidence: 99%
“…In Refs. [17,18], Liu et al produced a valence lattice QCD result which supports the Goldstone boson exchange picture, but Isgur pointed out that this is unjustified [15,16]. On the other hand, in the study of NN interactions on the quark level, the short-range feature can be explained by OGE interaction and quark exchange effect, while in the traditional one-boson exchange (OBE) model on the baryon level it comes from vector-meson (ρ, K * , ω, and φ) exchange.…”
Section: Introductionmentioning
confidence: 99%
“…They pointed out the spin-flavor interaction is important in explaining the energy of the Roper resonance and got a comparatively good fit to the baryon spectrum. However Isgur gave a critique of the boson exchange model and insisted that the OGE governs the baryon structure [15,16]. In Refs.…”
Section: Introductionmentioning
confidence: 99%
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“…The light quark is orbiting around this heavy source at a distance much larger (∼ 1/m q ) than the source size (∼ 2/m Q ). Thus the doubly heavy baryons look effectively like a two-body bound system and strongly resemble the heavy-light B and D mesons [2,13]. Then the HQET expansion in the inverse heavy quark mass can be used.…”
Section: Introductionmentioning
confidence: 99%