Hidden-Bottom Pentaquarks

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Hidden-Bottom Pentaquarks PHYSICAL REVIEW D 99, 014035 (2019) Hidden-bottom pentaquarks † ‡ Gang Yang,1,* Jialun Ping,2, and Jorge Segovia3, 1Department of Physics and State Key Laboratory of Low-Dimensional Quantum Physics, Tsinghua University, Beijing 100084, People’s Republic of China 2Department of Physics and Jiangsu Key Laboratory for Numerical Simulation of Large Scale Complex Systems, Nanjing Normal University, Nanjing 210023, People’s Republic of China 3Institut de Física d’Altes Energies (IFAE) and Barcelona Institute of Science and Technology (BIST), Universitat Autònoma de Barcelona, E-08193 Bellaterra (Barcelona), Spain (Received 19 September 2018; published 25 January 2019) The LHCb Collaboration has recently reported strong evidences of the existence of pentaquark states in þ þ the hidden-charm baryon sector, the so-called Pcð4380Þ and Pcð4450Þ signals. Five-quark bound states in the hidden-charm sector were explored by us using, for the quark-quark interaction, a chiral quark model which successfully explains meson and baryon phenomenology, from the light to the heavy quark sector. We extend herein such study into the hidden-bottom pentaquark sector, analyzing possible bound-states P 1Æ 3Æ 5Æ 1 3 with spin-parity quantum numbers J ¼ 2 , 2 and 2 , and in the 2 and 2 isospin sectors. We do not find positive parity hidden-bottom pentaquark states; however, several candidates with negative parity are found ΣðÞ ¯ ðÞ with dominant baryon-meson structures b B . Their inner structures have been also analyzed with the computation of the distance among any pair of quarks within the bound-state. This exercise reflects that molecular-type bound-states are favored when only color-singlet configurations are considered in the coupled-channels calculation whereas some deeply-bound compact pentaquarks can be found when hidden-color configurations are added. Finally, our findings resemble the ones found in the hidden-charm sector but, as expected, we find in the hidden-bottom sector larger binding energies and bigger contributions of the hidden-color configurations. DOI: 10.1103/PhysRevD.99.014035 I. INTRODUCTION In 2015, the LHCb Collaboration observed two ψ After decades of experimental and theoretical studies of hidden-charm pentaquark states in the J= p invariant Λ0 → ψ − hadrons, the conventional picture of mesons and baryons mass spectrum of the b J= K p decay [1]. One is ð4380Þþ ð4380 Æ 8 Æ 29Þ as, respectively, quark-antiquark and 3-quark bound states Pc with a mass of MeV and a ð205 Æ 18 Æ 86Þ ð4450Þþ is being left behind. On one hand, quantum chromody- width of MeV, and another is Pc ð4449 8 Æ 1 7 Æ 2 5Þ namics (QCD), the non-Abelian quantum field theory of with a mass of . MeV and a width of ð39 Æ 5 Æ 19Þ MeV. The preferred JP assignments are of the strong interactions, does not prevent to have exotic 3 5 hadrons such as glueballs, quark-gluon hybrids, and multi- opposite parity, with one state having spin 2 and the other 2. ð4380Þþ ð4450Þþ quark systems. On the other hand, more than two dozens of The discovery of the Pc and Pc has nontraditional charmonium- and bottomonium-like states, triggered many theoretical works on this kind of multiquark the so-called XYZ mesons, have been observed in the last systems. The interested reader is directed to the recent 15 years at B-factories (BABAR, Belle and CLEO), τ-charm review [2] on hidden-charm pentaquark and tetraquark facilities (CLEO-c and BESIII) and also proton-(anti) states in order to have a global picture of the current progress; however, one can highlight those theoretical proton colliders (CDF, D0, LHCb, ATLAS and CMS). þ þ studies of the Pcð4380Þ and Pcð4450Þ in which different kind of quark arrangements are used such as diquark- – – *[email protected] triquark [3 5], diquark-diquark-antiquark [3,6 11], and † [email protected] meson-baryon molecule [3,12–23]. It is also noteworthy ‡ [email protected] that some recent investigations have considered other possible physical mechanisms as the origin of the exper- Published by the American Physical Society under the terms of imental signals like kinematic effects and triangle singu- the Creative Commons Attribution 4.0 International license. – Further distribution of this work must maintain attribution to larities [24 28]. the author(s) and the published article’s title, journal citation, The observation of hadrons containing valence c-quarks and DOI. Funded by SCOAP3. is historically followed by the identification of similar 2470-0010=2019=99(1)=014035(11) 014035-1 Published by the American Physical Society GANG YANG, JIALUN PING, and JORGE SEGOVIA PHYS. REV. D 99, 014035 (2019) ¯ à ¯ à structures with b-quark content. Therefore, it is natural dominant ΣcD and ΣcD Fock-state components were also to expect a subsequent observation of the bottom analogues found in the region about 4.3–4.5 GeV. þ þ of the Pcð4380Þ and Pcð4450Þ resonances, if they All the details about our computational framework eventually exist. The LHCb Collaboration has recently will be described later but let us sketch here some of made an attempt (with negative result) to search for its main features. Our chiral quark model (ChQM) is pentaquark states containing a single b-quark, that decays based on the fact that chiral symmetry is spontaneously weakly via the b → ccs¯ transition, in the final states broken in QCD and, among other consequences, it pro- J=ψKþπ−p, J=ψK−π−p, J=ψK−πþp, and J=ψϕp [29]. vides a constituent quark mass to the light quarks. To Therefore, reports about similar explorations in other restore the chiral symmetry in the QCD Lagrangian, bottom pentaquark sectors like the hidden-bottom one, Goldstone-boson exchange interactions appear between should be expected in the near future. the light quarks. This fact is encoded in a phenomeno- Theoretical investigations of the spectrum of hidden- logical potential which already contains the perturbative bottom pentaquarks as well as their electromagnetic, one-gluon exchange (OGE) interaction and a nonperturba- strong and weak decays help in the experimental hunt tive linear-screened confining term.1 It is worthwhile to mentioned above. In addition to this, further theoretical note that chiral symmetry is explicitly broken in the heavy studies supply complementary information on the internal quark sector and this translates in our formalism to the fact structure and interquark interactions of pentaquarks with that the interaction terms between light-light, light-heavy ð4380Þþ heavy quark content. In Ref. [30], besides the Pc and heavy-heavy quarks are not the same, i.e., while state, the possible existence of hidden-bottom penta- Goldstone-boson exchanges are considered when the two quarks with a mass around 11.08–11.11 GeV and quan- quarks are light, they do not appear in the other two − tum numbers JP ¼ 3=2 was emphasized; it was also configurations: light-heavy and heavy-heavy; however, the indicated that there may exist some loosely-bound one-gluon exchange and confining potentials are flavor molecular-type pentaquarks in other heavy quark sectors. blindness. Ming-Zhu Liu et al. used heavy-quark symmetry argu- The five-body bound state problem is solved by means of ð4380Þ ð4450Þ ments to find the partners of the Pc and Pc the Gaußian expansion method (GEM) [43] which provides [31,32]. A quark model study of the baryo-quarkonium enough accuracy and simplifies the subsequent evaluation picture for hidden-charm and -bottom pentaquarks was of the matrix elements. As it is well know, the quark model recently released in Ref. [33] concluding that hidden- parameters are crucial in order to describe particular bottom pentaquarks are more likely to form than their physical observables. We have used values that have hidden-charm counterparts. The baryo-quarkonium pic- been fitted before through hadron [44–49], hadron-hadron ture has been also explored within a nonrelativistic [50–54] and multiquark [40,55,56] phenomenology. effective field theory approach in Refs. [34–36]. Finally, The structure of the present manuscript is organized in see also Refs. [37,38] for more information on the the following way. In Sec. II the ChQM, pentaquark wave- properties of the charmed and bottom pentaquark states functions and GEM are briefly presented and discussed. using the coupled-channel unitary approach, as well as Section III is devoted to the analysis and discussion on the Refs. [24,26,28,39] for illuminating discussions on the obtained results. We summarize and give some prospects structure of pentaquarks and their possible relation with in Sec. IV. triangle singularities. We study herein, within a chiral quark model formalism, II. THEORETICAL FRAMEWORK the possibility of having pentaquark bound-states in the P ¼ 1Æ 3Æ hidden-bottom sector with quantum numbers J 2 , 2 Although lattice QCD (LQCD) has made an impressive 5Æ 1 3 and 2 , and in the 2 and 2 isospin sectors. Their inner progress on understanding multiquark systems [57,58] and structures are also obtained by computing the distance the hadron-hadron interaction [59–61], the QCD-inspired among any pair of quarks within the bound-state. This quark models are still the main tool to shed some light on work is a natural extension of the analysis performed in the nature of the multiquark candidates observed by Ref. [40] in which similar structures were studied but in the experimentalists. þ hidden-charm sector. In Ref. [40], the Pcð4380Þ was The general form of our five-body Hamiltonian is given à ¯ suggested to be a bound state of ΣcD with quantum by [40] P ¼ 3− ð4450Þþ numbers J 2 whereas the nature of the Pc structure was not clearly established because, despite of X5 ⃗2 X5 ¼ þ pi − þ ð⃗ Þ ð Þ having a couple of possible candidates attending to the H mi TCM V rij ; 1 2mi agreement between theoretical and experimental masses, i¼1 j>i¼1 there was an inconsistency between the parity of the state determined experimentally and those predicted theoreti- 1The interested reader is referred to Refs.
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