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We calculate the full spectrum of D-wave states in the Upsilon system in lattice QCD for the first time, using an improved version of NonRelativistic QCD on coarse and fine "second generation" gluon field configurations from the MILC…

High Energy Physics - Lattice · Physics 2015-06-03 J. O. Daldrop , C. T. H. Davies , R. J. Dowdall

We use lattice QCD to investigate the existence of strong-interaction-stable antiheavy-antiheavy-light-light tetraquarks. We study the $\bar b \bar b u s$ system with quantum numbers $J^P = 1^+$ as well as the $\bar b \bar c u d$ systems…

High Energy Physics - Lattice · Physics 2022-08-23 Stefan Meinel , Martin Pflaumer , Marc Wagner

The bottomonium spectrum, consisting of bound states of a $b$ quark and an anti-$b$ quark, provides an excellent laboratory for probing quantum chromodynamics in the non-perturbative regime. While $S$ and $P$-wave bottomonium states are…

High Energy Physics - Experiment · Physics 2026-03-03 Belle II Collaboration , M. Abumusabh , I. Adachi , A. Aggarwal , L. Aggarwal , H. Ahmed , Y. Ahn , H. Aihara , S. Alghamdi , M. Alhakami , A. Aloisio , N. Althubiti , K. Amos , M. Angelsmark , N. Anh Ky , C. Antonioli , D. M. Asner , H. Atmacan , T. Aushev , R. Ayad , V. Babu , H. Bae , N. K. Baghel , S. Bahinipati , P. Bambade , Sw. Banerjee , M. Barrett , M. Bartl , J. Baudot , A. Baur , A. Beaubien , F. Becherer , 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 , M. -C. 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. Cochran , 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 , R. Dhayal , A. Di Canto , J. Dingfelder , Z. Doležal , I. Domínguez Jiménez , T. V. Dong , X. Dong , M. Dorigo , K. Dugic , G. Dujany , P. Ecker , D. Epifanov , J. Eppelt , R. Farkas , P. Feichtinger , T. Ferber , T. Fillinger , C. Finck , G. Finocchiaro , F. Forti , A. Frey , B. G. Fulsom , A. Gabrielli , A. Gale , E. Ganiev , 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 , B. Gobbo , R. Godang , W. Gradl , E. Graziani , D. Greenwald , Y. Guan , K. Gudkova , I. Haide , Y. Han , H. Hayashii , S. Hazra , C. Hearty , A. Heidelbach , G. Heine , I. Heredia de la Cruz , M. Hernández Villanueva , T. Higuchi , M. Hoek , M. Hohmann , R. Hoppe , P. Horak , C. -L. Hsu , T. Humair , T. Iijima , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , P. Jackson , D. Jacobi , W. W. Jacobs , E. -J. Jang , Q. P. Ji , S. Jia , Y. Jin , A. Johnson , J. Kandra , K. H. Kang , G. Karyan , F. Keil , C. Ketter , C. Kiesling , D. Y. Kim , H. Kim , J. -Y. Kim , K. -H. Kim , K. Kinoshita , P. Kodyš , T. Koga , S. Kohani , A. Korobov , S. Korpar , E. Kovalenko , R. Kowalewski , P. Križan , P. Krokovny , T. Kuhr , Y. Kulii , D. Kumar , R. Kumar , K. Kumara , S. Kurokawa , 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 , 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 , Z. Liptak , M. H. Liu , Q. Y. Liu , 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 , E. Manoni , M. Mantovano , D. Marcantonio , S. Marcello , M. Marfoli , C. Marinas , C. Martellini , A. Martens , T. Martinov , L. Massaccesi , M. Masuda , D. Matvienko , S. K. Maurya , M. Maushart , F. Mawas , J. A. McKenna , Z. Mediankin Gruberová , R. Mehta , F. Meier , D. Meleshko , M. Merola , C. Miller , M. Mirra , K. Miyabayashi , H. Miyake , R. Mizuk , G. B. Mohanty , S. Moneta , H. -G. Moser , Th. Muller , R. Mussa , I. Nakamura , M. Nakao , H. Nakazawa , Y. Nakazawa , M. Naruki , Z. Natkaniec , A. Natochii , M. Nayak , M. Neu , M. Niiyama , S. Nishida , R. Nomaru , A. Novosel , S. Ogawa , R. Okubo , H. Ono , F. Otani , P. Pakhlov , G. Pakhlova , A. Panta , S. Pardi , K. Parham , J. Park , K. 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 , A. Prakash , C. Praz , S. Prell , E. Prencipe , M. T. Prim , S. Privalov , I. Prudiiev , M. V. Purohit , H. Purwar , 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 , N. Rout , S. Saha , L. Salutari , D. A. Sanders , S. Sandilya , L. Santelj , C. Santos , V. Savinov , B. Scavino , S. Schneider , K. Schoenning , C. Schwanda , Y. Seino , K. Senyo , J. Serrano , M. E. Sevior , C. Sfienti , W. Shan , C. P. Shen , X. D. Shi , T. Shillington , T. Shimasaki , J. -G. Shiu , D. Shtol , 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 , S. Stefkova , R. Stroili , J. Strube , M. Sumihama , N. Suwonjandee , M. Takizawa , K. Tanida , F. Tenchini , F. Testa , A. Thaller , T. Tien Manh , O. Tittel , R. Tiwary , E. Torassa , K. Trabelsi , F. F. Trantou , I. Tsaklidis , I. Ueda , K. Unger , Y. Unno , K. Uno , S. Uno , 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 , Y. Xie , X. P. Xu , B. D. Yabsley , W. Yan , W. Yan , J. Yelton , K. Yi , J. H. Yin , K. Yoshihara , J. Yuan , Y. Yusa , L. Zani , F. Zeng , M. Zeyrek , B. Zhang , V. Zhilich , J. S. Zhou , Q. D. Zhou , L. Zhu , R. Žlebčík

Inspired by the newly observed $Z_{cs}^-(3985)$ by BESIII collaboration, we study the structure of this particle in the picture of $D_s^{(*)-}D^{(*)0}$ molecular state. Firstly we systematically construct the Lagrangians which describing…

High Energy Physics - Phenomenology · Physics 2020-11-19 Zhi-Feng Sun , Chu-Wen Xiao

We study the interaction of the doubly bottom systems $BB$, $B^* B$, $B_s B$, $B_s^* B$, $B^* B^*$, $B^* B_s$, $B^*B_s^*$, $B_s B_s$, $B_s B_s^*$, $B_s^* B_s^*$ by means of vector meson exchange with Lagrangians from an extension of the…

High Energy Physics - Phenomenology · Physics 2022-05-04 L. R. Dai , E. Oset , A. Feijoo , R. Molina , L. Roca , A. Martínez Torres , K. P. Khemchandani

We present a comprehensive theoretical study of the masses of possible baryonic and mesonic configurations containing a single top quark. Our analysis includes the baryons $\Lambda_t$, $\Xi_t$, $\Sigma_t$, $\Xi'_t$, $\Omega_t$,…

High Energy Physics - Phenomenology · Physics 2026-05-04 Z. Rajabi Najjar , M. Ahmadi , K. Azizi

Many mesons with properties incompatible with a $\bar cc$ structure have already been discovered, e.g. the $Z_c$ mesons with isospin 1. We investigate the spectrum of exotic charmonium-like mesons using lattice QCD. The focus is on $\bar cc…

High Energy Physics - Lattice · Physics 2022-12-12 Mitja Sadl , Sara Collins , M. Padmanath , Sasa Prelovsek

We present a lattice QCD calculation of the S-wave interactions between the spin-1/2 doubly charmed baryons ($\Xi_{cc},\Omega_{cc}$) and Goldstone bosons ($\pi,K,\bar{K}$) using the $N_f=2+1$ CLQCD ensembles with lattice spacing $a =…

High Energy Physics - Lattice · Physics 2025-09-30 Jing-Yu Yi , Ze-Rui Liang , Liuming Liu , De-Liang Yao

A lattice QCD study of the strong decay width and coupling constant of decuplet baryons to an octet baryon - pion state is presented. The transfer matrix method is used to obtain the overlap of lattice states with decuplet baryon quantum…

High Energy Physics - Lattice · Physics 2016-06-29 Constantia Alexandrou , John W. Negele , Marcus Petschlies , Andrew V. Pochinsky , Sergey N. Syritsyn

We report the ground state masses of hadrons containing at least one charm and one bottom quark using lattice quantum chromodynamics. These include mesons with spin (J)-parity (P) quantum numbers J(P): 0(-), 1(-), 1(+) and 0(+) and the…

High Energy Physics - Lattice · Physics 2018-11-30 Nilmani Mathur , M. Padmanath , Sourav Mondal

The \Lambda_c(2940)^+ baryon is studied in a constituent quark model as a molecular state composed by nucleons and D^* mesons. A bound state with the right binding energy is found for the J^\pi=3/2^- channel. The partial widths…

High Energy Physics - Phenomenology · Physics 2015-06-11 P. G. Ortega , D. R. Entem , F. Fernández

We use $n_f=2+1$ Wilson-clover gauge-field ensembles from the CLS consortium in a Lattice NRQCD setup to predict the binding energy of a $I(J^P)=0(1^+)$ $ud\bar{b}\bar{b}$ tetraquark and a $\frac{1}{2}(1^+)$ $\ell s\bar{b}\bar{b}$…

High Energy Physics - Lattice · Physics 2023-06-28 R. J. Hudspith , D. Mohler

Inspired by the latest experimental progress, we systematically study the OZI-allowed two-body strong decay properties of $1P$-, $1D$-, $2S$- and $2P$-wave $\Lambda_c$ baryons within the $j $-$j$ coupling scheme in the framework of the…

High Energy Physics - Phenomenology · Physics 2025-08-21 Yu-Bin Zhang , Li-Ye Xiao , Xian-Hui Zhong

We determine $J^{PC}=0^{++}$ and $2^{++}$ hadron-hadron scattering amplitudes in the charmonium energy region up to 4100 MeV using lattice QCD, a first-principles approach to QCD. Working at $m_\pi\approx 391$ MeV, more than 200…

High Energy Physics - Lattice · Physics 2024-08-07 David J. Wilson , Christopher E. Thomas , Jozef J. Dudek , Robert G. Edwards

Bound states of double-heavy tetraquarks are studied in a constituent quark model. Two bound states are found for isospin and spin-parity I(J^P ) = 0(1^+) in the bb\bar{u}\bar{d} channel. One is deeply bound and compact made of colored…

Nuclear Theory · Physics 2021-01-27 Q. Meng , E. Hiyama , A. Hosaka , M. Oka , P. Gubler , K. U. Can , T. T. Takahashi , H. S. Zong

In this paper it is proposed that the charged charmonium-like state $Z_c(3900)$ is a resonance above the threshold from the $D\bar{D}^*$ interaction. The $D\bar{D}^*$ interaction is described by the one-boson exchange model with light meson…

High Energy Physics - Phenomenology · Physics 2015-08-12 Jun He

We construct a potential obtained by one-pion exchange for the coupled channel $\Sigma_c^\ast$$\bar{D}$-$\Sigma_c$$\bar{D}^\ast$, and solve the coupled Schr\"{o}dinger equations to determine the binding energy. We find that there exists one…

High Energy Physics - Phenomenology · Physics 2016-06-15 Yuki Shimizu , Daiki Suenaga , Masayasu Harada

A new approach is presented to explore the singularity structure of lattice QCD in the complex chemical potential plane. Our method can be seen as a combination of the Taylor expansion and analytic continuation approaches. Its novelty lies…

The six quark state(uuddss) called H dibaryon($J^P=0^+$,$S=-2$) has been calculated to study its existence and stability. The simulations are performed in quenched QCD on $8^3 \times 24$ and $16^3 \times 48$ anisotropic lattices with…

High Energy Physics - Lattice · Physics 2008-11-26 Zhi-Huan Luo , Mushtaq Loan , Xiang-Qian Luo

Using the relativistic flux tube (RFT) model with spin-dependent corrections, we present a unified investigation of the mass spectra for singly bottom mesons ($B$, $B_s$) and doubly bottom baryons ($\Xi_{bb}$, $\Omega_{bb}$). Within this…

High Energy Physics - Phenomenology · Physics 2025-09-19 Pooja Jakhad , Ajay Kumar Rai