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Leptoquarks provide some of the simplest explanations to the hints of lepton flavor non-universality in $B$ decays. In particular, a new confining gauge group can provide a natural and appealing origin for the leptoquarks. So far, direct…

High Energy Physics - Phenomenology · Physics 2019-01-02 Angelo Monteux , Arvind Rajaraman

A general study of pentaquarks built with four quarks in a L=1 state and an antiquark in S-wave shows that several of such states are forbidden by a selection rule, which holds in the limit of flavour symmetry, to decay into a baryon and a…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. Buccella , P. Sorba

Dynamical calculations are performed for all members of the flavor antidecuplet to which the pentaquark $\Theta^+$ belongs. The framework is a constituent quark model where the short-range interaction has a flavor-spin structure. From…

High Energy Physics - Phenomenology · Physics 2017-08-23 Fl. Stancu

Assuming the two diquark structure for the pentaquark state as advocated in the Jaffe-Wilczek model, we study the strong decays of light and heavy parity-even pentaquark states using the light-front quark model in conjunction with the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hai-Yang Cheng , Chun-Khiang Chua

In this article, we present the scalar-diquark-scalar-diquark-antiquark type and scalar-diquark-axialvector-diquark-antiquark type pentaquark configurations in the diquark model, and study the masses and pole residues of the…

High Energy Physics - Phenomenology · Physics 2016-01-28 Zhi-Gang Wang , Tao Huang

In the framework of the color-magnetic interaction, we have systematically studied the mass splittings of the possible hidden-charm pentaquarks $qqqc\bar{c}$ ($q=u,d,s$) where the three light quarks are in a color-octet state. We find that…

High Energy Physics - Phenomenology · Physics 2017-02-07 Jing Wu , Yan-Rui Liu , Kan Chen , Xiang Liu , Shi-Lin Zhu

We propose a four-quark structure for some of the excited states of heavy mesons containing a single charm or bottom quark. The four-quark wave functions are constructed based on a diquark-antidiquark form under the constraint that they…

High Energy Physics - Phenomenology · Physics 2015-06-22 Hungchong Kim , Myung-Ki Cheoun , Yongseok Oh

Models proposed to explain recently discovered heavy-light four-quark states already assume certain internal structures, i.e. the (anti)quark constituents are grouped into diquark/antidiquark clusters, heavy-meson/light-meson clusters…

High Energy Physics - Phenomenology · Physics 2020-09-30 Paul C. Wallbott , Gernot Eichmann , Christian S. Fischer

States beyond those expected in the simple constituent quark model are now emerging. I focus on the scalar glueball and its mixing with states in the $q\bar{q}$ nonet, and also on correlations in Strong QCD that may form diquarks and seed…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. E. Close

The relativistic model of the ground state and excited heavy tetraquarks with hidden bottom is formulated within the diquark-antidiquark picture. The diquark structure is taken into account by calculating the diquark-gluon vertex in terms…

High Energy Physics - Phenomenology · Physics 2009-04-17 D. Ebert , R. N. Faustov , V. O. Galkin

Exotic antidecuplet baryons are predicted to be not only surprisingly light but also very narrow. First we explain how small decay width arises in the quark soliton model. Next, we study possible mixing of exotic antidecuplet with Roper…

High Energy Physics - Phenomenology · Physics 2011-01-25 Michal Praszalowicz

The observation of the two states $P_c(4380)$ and $P_c(4445)$ [Phys.Rev.Lett. 115 (2015) 072001] solids the existence of the pentaquark state in Nature. In this work, we study the spectrum of the pentaquark states including one or two heavy…

High Energy Physics - Phenomenology · Physics 2020-02-26 Ben-Teng Zhang , Jun-Shuai Wang , Yong-Liang Ma

Multiquark systems such as tetraquarks, pentaquarks and hexaquarks states are studied as di-hadronic molecules in a nonrelativistic model. The masses of several di-hadronic states using a molecular interaction provided by asymptotic…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ajay Kumar Rai , J N Pandya , P C Vinodkumar

A number of resonances comparable with a hypothesis of hidden-charm pentaquark is observed by the LHCb Collaboration. We interpret these narrow resonances as compact hidden-charm diquark-diquark-antiquark systems. Within this assumption, an…

High Energy Physics - Phenomenology · Physics 2023-10-03 Alexandra A. Dobrynina , Alexander Ya. Parkhomenko , Alexey V. Zinchenko

With the chiral quark model, we have calculated the axial charges of the pentaquark states with $(I,I_3)=(\frac{1}{2},\frac{1}{2})$ and $J^{P}=\frac{1}{2}^{\pm},\frac{3}{2}^{\pm},\frac{5}{2}^{\pm}$. The $P_c$ states with the same $J^P$…

High Energy Physics - Phenomenology · Physics 2017-01-04 Guang-Juan Wang , Zhan-Wei Liu , Shi-Lin Zhu

We analyze what consequences has the observation of exotic pentaquark baryons on the location of the non-exotic baryons belonging to the antidecuplet. We suggest that there must be a new nucleon state at 1650-1690 MeV and a new Sigma baryon…

High Energy Physics - Phenomenology · Physics 2009-11-10 Dmitri Diakonov , Victor Petrov

We introduce the hypothesis that diquarks and antidiquarks in tetraquarks are separated by a potential barrier. We show that this notion can answer satisfactorily long standing questions challenging the diquark-antidiquark model of exotic…

High Energy Physics - Phenomenology · Physics 2018-02-01 L. Maiani , A. D. Polosa , V. Riquer

In some models, exotic baryons with strangeness and anticharm or antibeauty should exist and even be stable against strong decay. We consider the stability of such possible exotic baryons, which in the constituent quark picture are called…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. B. Lichtenberg

We consider a $[ud]^2\bar{s}$ current in the QCD sum rule framework to study the mass of the recently observed pentaquark state $\Theta^+(1540)$, obtaining good agreement with the experimental value. We also study the mass of the pentaquark…

High Energy Physics - Phenomenology · Physics 2015-06-25 R. D. Matheus , F. S. Navarra , M. Nielsen , R. Rodrigues da Silva , S. H. Lee

The LHCb has discovered two new states with preferred $J^P$ quantum numbers $3/2^-$ and $5/2^+$ from $\Lambda_b$ decays. These new states can be interpreted as hidden charm pentaquarks. It has been argued that the main features of these…

High Energy Physics - Phenomenology · Physics 2016-01-27 Guan-Nan Li , Min He , Xiao-Gang He