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Related papers: Is $d^*(2380)$ a compact hexaquark state?

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We observe the radiative decay $D^{*}_{s0}(2317)^{+} \to D_{s}^{*+} \gamma$ for the first time, with a significance exceeding $10$ standard deviations. The signal is found in the continuum $e^+ e^- \to c\bar{c}$ process with the combined…

High Energy Physics - Experiment · Physics 2025-11-03 Belle II Collaboration , M. Abumusabh , I. Adachi , L. Aggarwal , H. Ahmed , Y. Ahn , H. Aihara , N. Akopov , S. Alghamdi , M. Alhakami , A. Aloisio , N. Althubiti , K. Amos , N. Anh Ky , C. Antonioli , D. M. Asner , H. Atmacan , T. Aushev , R. Ayad , V. Babu , N. K. Baghel , S. Bahinipati , P. Bambade , Sw. Banerjee , M. Barrett , M. Bartl , J. Baudot , A. Beaubien , J. Becker , J. V. Bennett , F. U. Bernlochner , V. Bertacchi , M. Bertemes , E. Bertholet , M. Bessner , S. Bettarini , F. Bianchi , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , A. Bondar , G. Bonvicini , J. Borah , A. Boschetti , A. Bozek , M. Bračko , P. Branchini , R. A. Briere , T. E. Browder , A. Budano , S. Bussino , Q. Campagna , M. Campajola , G. Casarosa , C. Cecchi , P. Chang , P. Cheema , L. Chen , B. G. Cheon , C. Cheshta , H. Chetri , K. Chilikin , K. Chirapatpimol , H. -E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , S. Choudhury , S. Chutia , J. A. Colorado-Caicedo , I. Consigny , L. Corona , J. X. Cui , E. De La Cruz-Burelo , S. A. De La Motte , G. De Nardo , G. De Pietro , R. de Sangro , M. Destefanis , S. Dey , A. Di Canto , Z. Doležal , I. Domínguez Jiménez , T. V. Dong , X. Dong , M. Dorigo , G. Dujany , P. Ecker , J. Eppelt , R. Farkas , P. Feichtinger , T. Ferber , T. Fillinger , C. Finck , G. Finocchiaro , F. Forti , B. G. Fulsom , A. Gabrielli , E. Ganiev , M. Garcia-Hernandez , R. Garg , G. Gaudino , V. Gaur , V. Gautam , A. Gaz , A. Gellrich , G. Ghevondyan , D. Ghosh , H. Ghumaryan , R. Giordano , A. Giri , P. Gironella Gironell , A. Glazov , B. Gobbo , R. Godang , O. Gogota , P. Goldenzweig , W. Gradl , E. Graziani , D. Greenwald , K. Gudkova , I. Haide , Y. Han , H. Hayashii , S. Hazra , C. Hearty , M. T. Hedges , G. Heine , I. Heredia de la Cruz , T. Higuchi , M. Hoek , M. Hohmann , R. Hoppe , P. Horak , X. T. Hou , C. -L. Hsu , A. Huang , T. Humair , T. Iijima , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , D. Jacobi , W. W. Jacobs , E. -J. Jang , Q. P. Ji , S. Jia , Y. Jin , A. Johnson , J. Kandra , K. H. Kang , S. Kang , G. Karyan , F. Keil , C. Kiesling , D. Y. Kim , J. -Y. Kim , K. -H. Kim , H. Kindo , K. Kinoshita , P. Kodyš , T. Koga , S. Kohani , A. Korobov , S. Korpar , E. Kovalenko , R. Kowalewski , P. Križan , P. Krokovny , T. Kuhr , D. Kumar , K. Kumara , T. Kunigo , A. Kuzmin , Y. -J. Kwon , S. Lacaprara , T. Lam , J. S. Lange , T. S. Lau , M. Laurenza , R. Leboucher , F. R. Le Diberder , H. Lee , M. J. Lee , C. Lemettais , P. Leo , P. M. Lewis , C. Li , H. -J. Li , L. K. Li , Q. M. Li , S. X. Li , W. Z. Li , Y. Li , Y. B. Li , Y. P. Liao , J. Libby , J. Lin , V. Lisovskyi , M. H. Liu , Q. Y. Liu , Z. Q. Liu , D. Liventsev , S. Longo , A. Lozar , T. Lueck , C. Lyu , J. L. Ma , Y. Ma , M. Maggiora , S. P. Maharana , R. Maiti , G. Mancinelli , R. Manfredi , M. Mantovano , D. Marcantonio , M. Marfoli , C. Marinas , C. Martellini , A. Martens , T. Martinov , L. Massaccesi , M. Masuda , D. Matvienko , M. Maushart , J. A. McKenna , Z. Mediankin Gruberová , R. Mehta , F. Meier , D. Meleshko , M. Merola , C. Miller , M. Mirra , H. Miyake , R. Mizuk , G. B. Mohanty , S. Moneta , H. -G. Moser , I. Nakamura , M. Nakao , M. Naruki , Z. Natkaniec , A. Natochii , M. Nayak , S. Nishida , R. Nomaru , S. Ogawa , H. Ono , F. Otani , G. Pakhlova , A. Panta , S. Pardi , K. Parham , J. Park , S. -H. Park , A. Passeri , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , M. Piccolo , L. E. Piilonen , P. L. M. Podesta-Lerma , T. Podobnik , C. Praz , S. Prell , M. T. Prim , S. Privalov , H. Purwar , P. Rados , S. Raiz , K. Ravindran , J. U. Rehman , M. Reif , S. Reiter , L. Reuter , D. Ricalde Herrmann , I. Ripp-Baudot , G. Rizzo , S. H. Robertson , J. M. Roney , A. Rostomyan , S. Saha , L. Salutari , D. A. Sanders , L. Santelj , C. Santos , V. Savinov , B. Scavino , S. Schneider , K. Schoenning , C. Schwanda , Y. Seino , K. Senyo , J. Serrano , C. Sfienti , W. Shan , G. Sharma , C. P. Shen , X. D. Shi , T. Shillington , J. -G. Shiu , D. Shtol , B. Shwartz , A. Sibidanov , F. Simon , J. Skorupa , R. J. Sobie , M. Sobotzik , A. Soffer , A. Sokolov , E. Solovieva , S. Spataro , K. Špenko , B. Spruck , M. Starič , P. Stavroulakis , R. Stroili , M. Sumihama , S. S. Tang , K. Tanida , F. Tenchini , F. Testa , A. Thaller , T. Tien Manh , O. Tittel , R. Tiwary , E. Torassa , K. Trabelsi , F. F. Trantou , I. Ueda , K. Unger , Y. Unno , K. Uno , S. Uno , P. Urquijo , Y. Ushiroda , S. E. Vahsen , R. van Tonder , K. E. Varvell , M. Veronesi , V. S. Vismaya , L. Vitale , V. Vobbilisetti , R. Volpe , M. Wakai , S. Wallner , M. -Z. Wang , A. Warburton , M. Watanabe , S. Watanuki , C. Wessel , E. Won , X. P. Xu , B. D. Yabsley , W. Yan , J. Yelton , K. Yi , J. H. Yin , K. Yoshihara , J. Yuan , Y. Yusa , L. Zani , M. Zeyrek , J. S. Zhou , Q. D. Zhou , L. Zhu , R. Žlebčík

Inspired by the experimental report by WASA-at-COSY Collaboration, we investigate the possibile existence of the dibaryon candidate $N\Delta$ with quantum numbers $IJ^P=21^+$ ($D_{21}$). The dynamical calculation shows that we cannot obtain…

High Energy Physics - Phenomenology · Physics 2018-09-12 Hongxia Huang , Xinmei Zhu , Jialun Ping , Fan Wang

We study the strong decay of $D_{s0}^*(2317)^+$ to $D_s^+ \pi^0$ considering the coupled channels of $D^0 K^+, D^+ K^0, D_s^+ \eta$ and $D_s^+ \pi^0$ within a picture for the interaction based on the local hidden gauge approach. We also…

High Energy Physics - Phenomenology · Physics 2026-03-17 Pei-Sen Su , Wen-Tao Lyu , Wei-Hong Liang , Eulogio Oset

Various theoretical calculations based on QCD or hadronic interactions predict that in addition to the recently observed dibaryon resonance $d^*(2380)$ with $I(J^P) = 0(3^+)$ there should also exist a dibaryon resonance with mirrored…

Recently, Belle Collaboration reported a new exotic state $Y(4620)$ with mass at 4625.9 MeV in the positronium annihilation process. Inspired by experiment, we study the tetraquark system $c\bar{s}s\bar{c}$ with quantum numbers…

High Energy Physics - Phenomenology · Physics 2020-03-18 Yue Tan , Jialun Ping

The resonance D*_sJ (2317) which is considered to be the 1^3P_0 state composed of charm and strange quarks has been discovered recently. The measured mass, which is about 160 MeV lower than the mass of the 1^3P_0 state obtained from the…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. S. Hwang , D. W. Kim

In a recent theoretical work, Phys. Lett. B785, 112 (2018), we proposed that a $K^*$ resonance with hidden charm content arises from the $KD\bar D^*$ dynamics, where the $D\bar D^*$ system is treated as a $Z_c(3900)$ or $X(3872)$. With the…

High Energy Physics - Phenomenology · Physics 2019-06-13 Xiu-Lei Ren , Brenda B. Malabarba , K. P. Khemchandani , A. Martinez Torres

The constituent quark model with color-spin hyperfine potential is used to investigate the property of a compact pentaquark configuration with $J^p$=$3/2^-$ and isospin=1/2, which is the most likely quantum number of one of the recently…

High Energy Physics - Phenomenology · Physics 2017-04-05 Woosung Park , Aaron Park , Sungtae Cho , Su Houng Lee

The decay widths of $\Upsilon(nS)$ $\rightarrow$ $\bar{d}^{\ast}(2380)+X$ with $n=1,2,3$ are studied in a phenomenological way. With the help of crossing symmetry, the decay widths are obtained by investigating the imaginary part of the…

High Energy Physics - Phenomenology · Physics 2018-05-17 Chao-Yi Lü , P. Wang , Y. B. Dong , P. N. Shen , Z. Y. Zhang , D. M. Li

Inspired by the report of D0 Collaboration on the state $X(5568)$ with four different flavors, a similar state, $ud\bar{s}\bar{b}$ is investigated in the present work. The advantage of looking for this state over the state $X(5568)$ with…

High Energy Physics - Phenomenology · Physics 2018-10-03 Xiaoyun Chen , Jialun Ping

The Babar and CLEO collaborations have recently observed states decaying to D_s^+\pi^0 and D_s^{*+}\pi^0 respectively and suggest the possible explanation that they are the missing P-wave c\bar{s} states with J^P=0^+ and 1^+. In this note…

High Energy Physics - Phenomenology · Physics 2010-04-05 Stephen Godfrey

In the framework of the quark delocalization color screening model (QDCSM), we systematically investigate the double-charm and double-strange tetraquark systems $cc\bar{s}\bar{s}$ with two structures: meson-meson and diquark-antidiquark.…

High Energy Physics - Phenomenology · Physics 2021-12-14 Yuheng Wu , Xin Jin , Runxin Liu , Hongxia Huang , Jialun Ping

We present our final results for the mass of the six quark flavor singlet state (J^P=0^+, S=-2) called H dibaryon, which would be the lightest possible strangelet in the context of strange quark matter. The calculations are performed in…

High Energy Physics - Lattice · Physics 2009-11-07 I. Wetzorke , F. Karsch

We study the decay widths of the narrow resonances $D_{sj}^*(2317)$ and $D_{sj}(2460)$ in the chiral quark model, together with the well-known $D^\ast$ and $D_s^*$ mesons. All the parameters in our calculation are taken from Godfrey and…

High Energy Physics - Phenomenology · Physics 2010-11-15 Feng-Lin Wang , Xiao-Lin Chen , Da-Hai Lu , Shi-Lin Zhu , Wei-Zhen Deng

We give a systematical study on the recently reported excited charm and charm-strange mesons with potential $1^-$ spin-parity, including the $D^*_{s1}(2700)^+$, $D^*_{s1}(2860)^+$, $D^*(2600)^0$, $D^*(2650)^0$, $D^*_1(2680)^0$ and…

High Energy Physics - Phenomenology · Physics 2021-11-05 Qiang Li , Yue Jiang , Tianhong Wang , Han Yuan , Guo-Li Wang , Chao-Hsi Chang

There exists experimental evidence that a dibaryon resonance d' with quantum numbers J^P=0^-,T=0 and mass 2065 MeV could be the origin of the narrow peak in the (\pi^+ ,\pi^- ) double charge exchange cross--sections on nuclei. We…

Nuclear Theory · Physics 2016-09-08 Georg Wagner , L. Ya. Glozman , A. J. Buchmann , Amand Faessler

QCD instantons are known to produce deeply bound diquarks. We study whether it may be used as building blocks in the formation of multiquark states, in particular pentaquarks and dibaryons. A simple model is presented in which the lowest…

High Energy Physics - Phenomenology · Physics 2016-09-06 E. V. Shuryak

The width of three-body single-pion decay process $d^*\to NN\pi^{0,\pm}$ is calculated by using the $d^*$ wave function obtained from our chiral SU(3) constituent quark model calculation. The effect of the dynamical structure on the width…

Nuclear Theory · Physics 2017-04-05 Yubing Dong , Fei Huang , Pengnian Shen , Zongye Zhang

The recently discovered charmed-strangemeson Ds0*(2317) has been speculated to be a tetraquark mesonium. We study this suggestion with overlap fermions on 2+1 flavor domain wall fermion configurations. We use 4-quark interpolating…

High Energy Physics - Lattice · Physics 2011-05-02 M. Gong , A. Li , A. Alexandru , Y. Chen , T. Draper , K. F. Liu

Recently, a charmonium $X(3960)$ in $B$ decays in the $D_s^+D_s^-$ invariant-mass spectrum is discovered by the LHCb Collaboration with the quantum number $J^{PC}=0^{++}$. Motivated by the discovery, in this work, we systematically…

High Energy Physics - Phenomenology · Physics 2025-02-18 Xiaoyun Chen , Yue Tan , Xuejie Liu , Jialun Ping
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