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On a possibility of exotic heavy baryons
High Energy Physics - Phenomenology · Submitted 20 May 2018
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We argue that three of the LHCb resonances are parity ($-$) excitations of the ground state SU(3) sextets, while the other two with the smallest widths are exotic pentaquarks that belong to the SU(3) $\overline{\mathbf{15}}$.
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The abstract, sentence by sentence
Triggered by a recent announcement by the LHCb Collaboration of five excited $\Omega^0_c$ resonances of small widths we propose an interpretation based on the Chiral Quark Soliton Model. We argue that three of the LHCb resonances are parity ($-$) excitations of the ground state SU(3) sextets, while the other two with the smallest widths are exotic pentaquarks that belong to the SU(3) $\overline{\mathbf{15}}$. We first briefly review the model and discuss the status of the putative $\Theta^+(1540)$. Next we show how to generalize the model to the case of heavy baryons. We test this approach against the ground state $\overline{\mathbf{3}}$ and ${\mathbf{6}}$ heavy baryons, and discuss different excitations that are possible in the Chiral Quark Soliton Model. We show that the model accommodates two excited $\overline{\mathbf{3}}$ in the charm sector that are experimentally observed. Finally we discuss possible assignments of the LHCb $\Omega^0_c$ states.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Triggered by a recent announcement by the LHCb Collaboration of five excited $\Omega^0_c$ resonances of small widths we propose an interpretation based on the Chiral Quark Soliton Model. | contribution 0.55 | 0.30 | 0.09 | hedged possibility 0.40 |
| s1 | We argue that three of the LHCb resonances are parity ($-$) excitations of the ground state SU(3) sextets, while the other two with the smallest widths are exotic pentaquarks that belong to the SU(3) $\overline{\mathbf{15}}$. | interpretation 0.85 | 0.59 | 0.87 | asserted 0.81 |
| s2 | We first briefly review the model and discuss the status of the putative $\Theta^+(1540)$. | method 0.46 | 0.30 | 0.02 | unclear 0.62 |
| s3 | Next we show how to generalize the model to the case of heavy baryons. | method 0.70 | 0.77 | 0.02 | asserted 0.91 |
| s4 | We test this approach against the ground state $\overline{\mathbf{3}}$ and ${\mathbf{6}}$ heavy baryons, and discuss different excitations that are possible in the Chiral Quark Soliton Model. | method 0.64 | 0.90 | 0.04 | asserted 0.89 |
| s5 | We show that the model accommodates two excited $\overline{\mathbf{3}}$ in the charm sector that are experimentally observed. | result 0.99 | 0.88 | 0.08 | asserted 1.00 |
| s6 | Finally we discuss possible assignments of the LHCb $\Omega^0_c$ states. | contribution 0.68 | 0.72 | 0.15 | hedged possibility 0.61 |
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The paper
Original abstract
Triggered by a recent announcement by the LHCb Collaboration of five excited $\Omega^0_c$ resonances of small widths we propose an interpretation based on the Chiral Quark Soliton Model. We argue that three of the LHCb resonances are parity ($-$) excitations of the ground state SU(3) sextets, while the other two with the smallest widths are exotic pentaquarks that belong to the SU(3) $\overline{\mathbf{15}}$. We first briefly review the model and discuss the status of the putative $\Theta^+(1540)$. Next we show how to generalize the model to the case of heavy baryons. We test this approach against the ground state $\overline{\mathbf{3}}$ and ${\mathbf{6}}$ heavy baryons, and discuss different excitations that are possible in the Chiral Quark Soliton Model. We show that the model accommodates two excited $\overline{\mathbf{3}}$ in the charm sector that are experimentally observed. Finally we discuss possible assignments of the LHCb $\Omega^0_c$ states.
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How the literature uses it
2 arXiv papers cite this in 3 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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We argue that it is not possible to accommodate all five $\Omega_c$'s within five parity minus excitations predicetd by the model and propose to interpret two narrowest states split by 70 MeV as pentaquarks belonging to the SU(3) representation $\overline{15}$.
Papers citing it · 2 sentences without a confident label
Cites it as background 1 paper
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Other possible interpretations of these states are summarised in Ref. [ref] .
Heavy baryon decay widths in the large $N_c$ limit in chiral theory · Introduction · 0.98
What it cites · 3 sentences without a confident label
Cites as background 7 papers
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In Refs. [ref] the new states are treated as bound states of a charm quark and a light diquark, the authors of Refs. [ref] interpreted the new states as molecular states and in some approaches [ref] as pentaquarks.
Possible open-charmed pentaquark molecule $\Omega_c(3188)$ --- the $D \Xi$ bound state --- in the Bethe-Salpeter formalism · Introduction · 0.96
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In Refs. [ref] the new states are treated as bound states of a charm quark and a light diquark, the authors of Refs. [ref] interpreted the new states as molecular states and in some approaches [ref] as pentaquarks.
Possible pentaquark candidates: new excited $\Omega_c$ states · Introduction · 0.96
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Decay properties of these states have been studied in a $^3P_0$ model [ref] , quark potential models [ref] , chiral quark model [ref] and in molecular model [ref] .
Strong and radiative decays of D\Xi molecular state and newly observed $\Omega_c$ states · Introduction · 0.97
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