2020
DOI: 10.3390/particles3010019
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Heavy Baryon Spectroscopy in the Relativistic Quark Model

Abstract: Masses of heavy baryons are calculated in the framework of the relativistic quark-diquark picture and QCD. The obtained results are in good agreement with available experimental data including recent measurements by the LHCb Collaboration. Possible quantum numbers of excited heavy baryon states are discussed.

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Cited by 17 publications
(9 citation statements)
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“…[72,73] applied the light cone QCD sum rules to study its decays to ground-state bottom baryons and a meson considering the heavy quark effective theory. The consistency of the quantum numbers of the Ξ b (6227) − with a P -wave state with J P = 1 2 − , 3 2 − and 5 2 − was also indicated by mass calculation in the quark-diquark picture [74,75]. In another work made in the quark-diquark picture, the preferable spin of this particle was stated to be J P = 3 2 − [76].…”
Section: Introductionmentioning
confidence: 75%
“…[72,73] applied the light cone QCD sum rules to study its decays to ground-state bottom baryons and a meson considering the heavy quark effective theory. The consistency of the quantum numbers of the Ξ b (6227) − with a P -wave state with J P = 1 2 − , 3 2 − and 5 2 − was also indicated by mass calculation in the quark-diquark picture [74,75]. In another work made in the quark-diquark picture, the preferable spin of this particle was stated to be J P = 3 2 − [76].…”
Section: Introductionmentioning
confidence: 75%
“…Only for particles with S = T = 1:5 and S = T = 4:4 is this perturbative energy of order 1 zero, and such particles do not physically exist. Table 4 presents our results as compared to the results from the nonrelativistic method [30] and lattice QCD calculations [31,32]. As observed, there is a good agreement between the two sets of results.…”
Section: Screened Potentialmentioning
confidence: 60%
“…[72,73] applied the light cone QCD sum rules to study its decays to ground-state bottom baryons and a meson considering the heavy quark effective theory. The consistency of the quantum numbers of the Ξ b (6227) − with a P -wave state with J P = 1 2 − , 3 2 − and 5 2 − was also indicated by mass calculation in the quark-diquark picture [74,75]. In another work made in the quark-diquark picture, the preferable spin of this particle was stated to be J P = 3 2 − [76].…”
Section: Introductionmentioning
confidence: 75%