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Related papers: Analysis of the $\Lambda_c(2625)$ and $\Xi_c(2815)…

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We present a study of baryon ground states and low lying excitations of non-strange and strange baryons. The results are based on seven gauge field ensembles with two dynamical light Chirally Improved (CI) quarks corresponding to pion…

High Energy Physics - Lattice · Physics 2015-06-12 Georg P. Engel , C. B. Lang , Daniel Mohler , Andreas Schaefer

Stimulated by the observation of $\Lambda_c(2910)^+$ by the Belle Collaboration, the $S$-wave $qqq\bar{q}c~(q=u~\text{or}~d)$ pentaquark systems with $I$ = 0, $J^P$ = $\frac{1}{2}^-,~\frac{3}{2}^- and~\frac{5}{2}^-$ are investigated in the…

High Energy Physics - Phenomenology · Physics 2022-11-23 Ye Yan , Xiaohuang Hu , Yuheng Wu , Hongxia Huang , Jialun Ping , Youchang Yang

In this article, we study the mass spectrum of the scalar hidden charm and bottom tetraquark states with the QCD sum rules. The numerical results are compared with the corresponding ones from a relativistic quark model based on a…

High Energy Physics - Phenomenology · Physics 2010-04-23 Zhi-Gang Wang

In this article, we study the doubly heavy baryon states and pentaquark states with the QCD sum rules by carrying out the operator product expansion up to the vacuum condensates of dimension $7$ and $13$ respectively in a consistent way. In…

High Energy Physics - Phenomenology · Physics 2018-10-17 Zhi-Gang Wang

In the present work, we construct eight six-quark currents to study the $\Sigma_c\bar{\Sigma}_c$ baryonium and $\Sigma_c\Sigma_c$ dibaryon states via the QCD sum rules. For either $\Sigma_c\bar{\Sigma}_c$ baryonium or $\Sigma_c\Sigma_c$…

High Energy Physics - Phenomenology · Physics 2022-05-03 Xiu-Wu Wang , Zhi-Gang Wang

We investigate the possible existence of double-strangeness hidden-charm pentaquark states, denoted as $P_{c\bar{c}ss}$, within an off-shell coupled-channel formalism. Eleven meson-baryon channels with total strangeness $S = -2$ are…

High Energy Physics - Phenomenology · Physics 2025-08-25 Samson Clymton , Hyun-Chul Kim , Terry Mart

We present a coupled channel unitary approach to obtain states dynamically generated from the meson baryon interaction with hidden charm, using constraints of heavy quark spin symmetry. We use as basis of states, $\bar D B$, $\bar D^* B$…

High Energy Physics - Phenomenology · Physics 2013-09-18 C. W. Xiao , J. Nieves , E. Oset

Inspired by $P_c(4380)$ and $P_c(4450)$ recently observed by LHCb, a QCD sum rule investigation is performed, by which they can be identified as exotic hidden-charm pentaquarks composed of an anti-charmed meson and a charmed baryon. Our…

High Energy Physics - Phenomenology · Physics 2015-10-21 Hua-Xing Chen , Wei Chen , Xiang Liu , T. G. Steele , Shi-Lin Zhu

We give the explicit wave functions of the $qqqq\bar{q}$ components of the C=+1, J=1/2 charmed baryons, $\Sigma_{c}$, $\Lambda_{c}$ and $\Xi_{c}^{a}$, and calculate the magnetic moments by adding the 5q components contributions, and we also…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chun-Sheng An

A search for the doubly charmed baryon Xi_cc^+ in the decay mode Xi_cc^+ -> Lambda_c^+ K^- pi^+ is performed with a data sample, corresponding to an integrated luminosity of 0.65/fb, of pp collisions recorded at a centre-of-mass energy of 7…

High Energy Physics - Experiment · Physics 2016-03-27 LHCb collaboration , R. Aaij , B. Adeva , M. Adinolfi , C. Adrover , A. Affolder , Z. Ajaltouni , J. Albrecht , F. Alessio , M. Alexander , S. Ali , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , S. Amerio , Y. Amhis , L. Anderlini , J. Anderson , R. Andreassen , J. E. Andrews , R. B. Appleby , O. Aquines Gutierrez , F. Archilli , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , M. Baalouch , S. Bachmann , J. J. Back , A. Badalov , C. Baesso , V. Balagura , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , Th. Bauer , A. Bay , J. Beddow , F. Bedeschi , I. Bediaga , S. Belogurov , K. Belous , I. Belyaev , E. Ben-Haim , G. Bencivenni , S. Benson , J. Benton , A. Berezhnoy , R. Bernet , M. -O. Bettler , M. van Beuzekom , A. Bien , S. Bifani , T. Bird , A. Bizzeti , P. M. Bjørnstad , T. Blake , F. Blanc , J. Blouw , S. Blusk , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , A. Borgia , T. J. V. Bowcock , E. Bowen , C. Bozzi , T. Brambach , J. van den Brand , J. Bressieux , D. Brett , M. Britsch , T. Britton , N. H. Brook , H. Brown , A. Bursche , G. Busetto , J. Buytaert , S. Cadeddu , O. Callot , M. Calvi , M. Calvo Gomez , A. Camboni , P. Campana , D. Campora Perez , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , H. Carranza-Mejia , L. Carson , K. Carvalho Akiba , G. Casse , L. Castillo Garcia , M. Cattaneo , Ch. Cauet , R. Cenci , M. Charles , Ph. Charpentier , S. -F. Cheung , N. Chiapolini , M. Chrzaszcz , K. Ciba , X. Cid Vidal , G. Ciezarek , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , C. Coca , V. Coco , J. Cogan , E. Cogneras , P. Collins , A. Comerma-Montells , A. Contu , A. Cook , M. Coombes , S. Coquereau , G. Corti , B. Couturier , G. A. Cowan , D. C. Craik , M. Cruz Torres , S. Cunliffe , R. Currie , C. D'Ambrosio , P. David , P. N. Y. David , A. Davis , I. De Bonis , K. De Bruyn , S. De Capua , M. De Cian , J. M. De Miranda , L. De Paula , W. De Silva , P. De Simone , D. Decamp , M. Deckenhoff , L. Del Buono , N. Déléage , D. Derkach , O. Deschamps , F. Dettori , A. Di Canto , H. Dijkstra , M. Dogaru , S. Donleavy , F. Dordei , A. Dosil Suárez , D. Dossett , A. Dovbnya , F. Dupertuis , P. Durante , R. Dzhelyadin , A. Dziurda , A. Dzyuba , S. Easo , U. Egede , V. Egorychev , S. Eidelman , D. van Eijk , S. Eisenhardt , U. Eitschberger , R. Ekelhof , L. Eklund , I. El Rifai , Ch. Elsasser , A. Falabella , C. Färber , C. Farinelli , S. Farry , D. Ferguson , V. Fernandez Albor , F. Ferreira Rodrigues , M. Ferro-Luzzi , S. Filippov , M. Fiore , C. Fitzpatrick , M. Fontana , F. Fontanelli , R. Forty , O. Francisco , M. Frank , C. Frei , M. Frosini , E. Furfaro , A. Gallas Torreira , D. Galli , M. Gandelman , P. Gandini , Y. Gao , J. Garofoli , P. Garosi , J. Garra Tico , L. Garrido , C. Gaspar , R. Gauld , E. Gersabeck , M. Gersabeck , T. Gershon , Ph. Ghez , V. Gibson , L. Giubega , V. V. Gligorov , C. Göbel , D. Golubkov , A. Golutvin , A. Gomes , P. Gorbounov , H. Gordon , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , G. Graziani , A. Grecu , E. Greening , S. Gregson , P. Griffith , L. Grillo , O. Grünberg , B. Gui , E. Gushchin , Yu. Guz , T. Gys , C. Hadjivasiliou , G. Haefeli , C. Haen , S. C. Haines , S. Hall , B. Hamilton , T. Hampson , S. Hansmann-Menzemer , N. Harnew , S. T. Harnew , J. Harrison , T. Hartmann , J. He , T. Head , V. Heijne , K. Hennessy , P. Henrard , J. A. Hernando Morata , E. van Herwijnen , M. Heß , A. Hicheur , E. Hicks , D. Hill , M. Hoballah , C. Hombach , W. Hulsbergen , P. Hunt , T. Huse , N. Hussain , D. Hutchcroft , D. Hynds , V. Iakovenko , M. Idzik , P. Ilten , R. Jacobsson , A. Jaeger , E. Jans , P. Jaton , A. Jawahery , F. Jing , M. John , D. Johnson , C. R. Jones , C. Joram , B. Jost , M. Kaballo , S. Kandybei , W. Kanso , M. Karacson , T. M. Karbach , I. R. Kenyon , T. Ketel , B. Khanji , O. Kochebina , I. Komarov , R. F. Koopman , P. Koppenburg , M. Korolev , A. Kozlinskiy , L. Kravchuk , K. Kreplin , M. Kreps , G. Krocker , P. Krokovny , F. Kruse , M. Kucharczyk , V. Kudryavtsev , K. Kurek , T. Kvaratskheliya , V. N. La Thi , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , R. W. Lambert , E. Lanciotti , G. Lanfranchi , C. Langenbruch , T. Latham , C. Lazzeroni , R. Le Gac , J. van Leerdam , J. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , S. Leo , O. Leroy , T. Lesiak , B. Leverington , Y. Li , L. Li Gioi , M. Liles , R. Lindner , C. Linn , B. Liu , G. Liu , S. Lohn , I. Longstaff , J. H. Lopes , N. Lopez-March , H. Lu , D. Lucchesi , J. Luisier , H. Luo , O. Lupton , F. Machefert , I. V. Machikhiliyan , F. Maciuc , O. Maev , S. Malde , G. Manca , G. Mancinelli , J. Maratas , U. Marconi , P. Marino , R. Märki , J. Marks , G. Martellotti , A. Martens , A. Martín Sánchez , M. Martinelli , D. Martinez Santos , D. Martins Tostes , A. Martynov , A. Massafferri , R. Matev , Z. Mathe , C. Matteuzzi , E. Maurice , A. Mazurov , J. McCarthy , A. McNab , R. McNulty , B. McSkelly , B. Meadows , F. Meier , M. Meissner , M. Merk , D. A. Milanes , M. -N. Minard , J. Molina Rodriguez , S. Monteil , D. Moran , P. Morawski , A. Mordà , M. J. Morello , R. Mountain , I. Mous , F. Muheim , K. Müller , R. Muresan , B. Muryn , B. Muster , P. Naik , T. Nakada , R. Nandakumar , I. Nasteva , M. Needham , S. Neubert , N. Neufeld , A. D. Nguyen , T. D. Nguyen , C. Nguyen-Mau , M. Nicol , V. Niess , R. Niet , N. Nikitin , T. Nikodem , A. Nomerotski , A. Novoselov , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , S. Ogilvy , O. Okhrimenko , R. Oldeman , M. Orlandea , J. M. Otalora Goicochea , P. Owen , A. Oyanguren , B. K. Pal , A. Palano , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , C. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , G. N. Patrick , C. Patrignani , C. Pavel-Nicorescu , A. Pazos Alvarez , A. Pearce , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , E. Perez Trigo , A. Pérez-Calero Yzquierdo , P. Perret , M. Perrin-Terrin , L. Pescatore , E. Pesen , G. Pessina , K. Petridis , A. Petrolini , A. Phan , E. Picatoste Olloqui , B. Pietrzyk , T. Pilař , D. Pinci , S. Playfer , M. Plo Casasus , F. Polci , G. Polok , A. Poluektov , E. Polycarpo , A. Popov , D. Popov , B. Popovici , C. Potterat , A. Powell , J. Prisciandaro , A. Pritchard , C. Prouve , V. Pugatch , A. Puig Navarro , G. Punzi , W. Qian , B. Rachwal , J. H. Rademacker , B. Rakotomiaramanana , M. S. Rangel , I. Raniuk , N. Rauschmayr , G. Raven , S. Redford , S. Reichert , M. M. Reid , A. C. dos Reis , S. Ricciardi , A. Richards , K. Rinnert , V. Rives Molina , D. A. Roa Romero , P. Robbe , D. A. Roberts , A. B. Rodrigues , E. Rodrigues , P. Rodriguez Perez , S. Roiser , V. Romanovsky , A. Romero Vidal , M. Rotondo , J. Rouvinet , T. Ruf , F. Ruffini , H. Ruiz , P. Ruiz Valls , G. Sabatino , J. J. Saborido Silva , N. Sagidova , P. Sail , B. Saitta , V. Salustino Guimaraes , B. Sanmartin Sedes , R. Santacesaria , C. Santamarina Rios , E. Santovetti , M. Sapunov , A. Sarti , C. Satriano , A. Satta , M. Savrie , D. Savrina , M. Schiller , H. Schindler , M. Schlupp , M. Schmelling , B. Schmidt , O. Schneider , A. Schopper , M. -H. Schune , R. Schwemmer , B. Sciascia , A. Sciubba , M. Seco , A. Semennikov , K. Senderowska , I. Sepp , N. Serra , J. Serrano , P. Seyfert , M. Shapkin , I. Shapoval , Y. Shcheglov , T. Shears , L. Shekhtman , O. Shevchenko , V. Shevchenko , A. Shires , R. Silva Coutinho , M. Sirendi , N. Skidmore , T. Skwarnicki , N. A. Smith , E. Smith , E. Smith , J. Smith , M. Smith , M. D. Sokoloff , F. J. P. Soler , F. Soomro , D. Souza , B. Souza De Paula , B. Spaan , A. Sparkes , P. Spradlin , F. Stagni , S. Stahl , O. Steinkamp , S. Stevenson , S. Stoica , S. Stone , B. Storaci , M. Straticiuc , U. Straumann , V. K. Subbiah , L. Sun , W. Sutcliffe , S. Swientek , V. Syropoulos , M. Szczekowski , P. Szczypka , D. Szilard , T. Szumlak , S. T'Jampens , M. Teklishyn , E. Teodorescu , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , S. Tolk , D. Tonelli , S. Topp-Joergensen , N. Torr , E. Tournefier , S. Tourneur , M. T. Tran , M. Tresch , A. Tsaregorodtsev , P. Tsopelas , N. Tuning , M. Ubeda Garcia , A. Ukleja , A. Ustyuzhanin , U. Uwer , V. Vagnoni , G. Valenti , A. Vallier , R. Vazquez Gomez , P. Vazquez Regueiro , C. Vázquez Sierra , S. Vecchi , J. J. Velthuis , M. Veltri , G. Veneziano , M. Vesterinen , B. Viaud , D. Vieira , X. Vilasis-Cardona , A. Vollhardt , D. Volyanskyy , D. Voong , A. Vorobyev , V. Vorobyev , C. Voß , H. Voss , R. Waldi , C. Wallace , R. Wallace , S. Wandernoth , J. Wang , D. R. Ward , N. K. Watson , A. D. Webber , D. Websdale , M. Whitehead , J. Wicht , J. Wiechczynski , D. Wiedner , L. Wiggers , G. Wilkinson , M. P. Williams , M. Williams , F. F. Wilson , J. Wimberley , J. Wishahi , W. Wislicki , M. Witek , G. Wormser , S. A. Wotton , S. Wright , S. Wu , K. Wyllie , Y. Xie , Z. Xing , Z. Yang , X. Yuan , O. Yushchenko , M. Zangoli , M. Zavertyaev , F. Zhang , L. Zhang , W. C. Zhang , Y. Zhang , A. Zhelezov , A. Zhokhov , L. Zhong , A. Zvyagin

The masses of the low lying baryons are evaluated using a total of ten ensembles of dynamical twisted mass fermion gauge configurations. The simulations are performed using two degenerate flavors of light quarks, and a strange and a charm…

High Energy Physics - Lattice · Physics 2015-06-22 C. Alexandrou , V. Drach , K. Jansen , C. Kallidonis , G. Koutsou

We construct, in the work, chiral $SU(3)$ Lagrangian with $D$ mesons of spin $J^P=0^-$ and $J^P=1^-$ and charmed baryons of spin $J^P=1/2^+$ and $J^P=3/2^+$. There are 42 leading two-body counter-terms involving two charmed baryon fields…

High Energy Physics - Phenomenology · Physics 2016-06-15 Daris Samart , Chakrit Nualchimplee , Yupeng Yan

The methods of QCD sum rules and light-cone sum rules within the framework of heavy quark effective theory have been widely applied to study the singly heavy baryons, and especially, we have applied these methods to predict not only the…

High Energy Physics - Phenomenology · Physics 2024-04-11 Wei-Han Tan , Hui-Min Yang , Hua-Xing Chen

I suggest that the conventional assignment of quantum numbers to the observed charm and bottom baryons is not correct, as these assignments imply large violation of the heavy spin-flavor and light $SU(3)$ symmetries. I propose an…

High Energy Physics - Phenomenology · Physics 2009-10-28 Adam F. Falk

We use QCD sum rules to study the possible existence of $QQ-\bar{u}\bar{d}$ mesons, assumed to be a state with $J^{P}=1^{+}$. For definiteness, we work with a current with an axial heavy diquark and a scalar light antidiquark, at leading…

High Energy Physics - Phenomenology · Physics 2008-11-26 Fernando S. Navarra , Marina Nielsen , Su Houng Lee

We present the results of a lattice calculation of four-quark states with the quark contents $\bar{b}\bar{c}q_1q_2$ where $q_1,q_2 \in u,d,s$. For the spin 1 states, when the light quark ($q_1, q_2$) masses are lighter, we find at least one…

High Energy Physics - Lattice · Physics 2021-11-03 M. Padmanath , Nilmani Mathur

We observe a signal for the doubly charmed baryon Xi_cc^+ in the charged decay mode Xi_cc^+ --> Lambda_c^+ K- pi+ in data from SELEX, the charm hadro-production experiment at Fermilab. We observe an excess of 15.9 events over an expected…

High Energy Physics - Experiment · Physics 2008-11-26 The SELEX Collaboration , M. Mattson

Low-lying $\Lambda$ baryons with spin 1/2 are analyzed in full (unquenched) lattice QCD. We construct $2 \times 2$ cross correlators from flavor SU(3) "octet" and "singlet" baryon operators, and diagonalize them so as to extract information…

High Energy Physics - Lattice · Physics 2010-04-30 Toru T. Takahashi , Makoto Oka

In heavy quark limit, the lowest-lying charmed baryons with two light quarks can form an SU(3) triplet and sextet. The $\Xi_c$ in the SU(3) triplet and $\Xi_c'$ in the sextet have the same $J^{PC}$ quantum number and can mix due to the…

High Energy Physics - Lattice · Physics 2023-05-31 Hang Liu , Liuming Liu , Peng Sun , Wei Sun , Jin-Xin Tan , Wei Wang , Yi-Bo Yang , Qi-An Zhang

The decays of the ground-state charmed baryon $\Lambda_c$ are now close to being completely mapped out. In this paper we discuss some remaining open questions, whose answers can help shed light on weak processes contributing to those…

High Energy Physics - Phenomenology · Physics 2018-06-27 Michael Gronau , Jonathan L. Rosner
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