English
Related papers

Related papers: Hidden charm dynamically generated resonances and …

200 papers

Two new states in the charm strange sector, DsJ(2317) and DsJ(2460), have recently been discovered at electron positron collider experiments. The new states are first observed in the dominant Ds pi0 and Ds* pi0 modes respectively and are…

High Energy Physics - Experiment · Physics 2010-11-15 Jianchun Wang

We propose a new algorithm for the identification of the production flavor of neutral $D$ mesons in the Belle II experiment. The algorithm exploits the correlation between the flavor of a reconstructed neutral $D$ meson (signal $D$ meson)…

High Energy Physics - Experiment · Physics 2023-07-03 Belle II Collaboration , I. Adachi , L. Aggarwal , H. Ahmed , H. Aihara , N. Akopov , A. Aloisio , N. Anh Ky , D. M. Asner , H. Atmacan , T. Aushev , V. Aushev , M. Aversano , V. Babu , H. Bae , S. Bahinipati , P. Bambade , Sw. Banerjee , M. Barrett , J. Baudot , M. Bauer , A. Baur , A. Beaubien , J. Becker , P. K. Behera , J. V. Bennett , F. U. Bernlochner , V. Bertacchi , M. Bertemes , E. Bertholet , M. Bessner , S. Bettarini , B. Bhuyan , F. Bianchi , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , A. Bolz , A. Bondar , J. Borah , A. Bozek , M. Bračko , P. Branchini , R. A. Briere , T. E. Browder , A. Budano , S. Bussino , M. Campajola , L. Cao , G. Casarosa , C. Cecchi , J. Cerasoli , M. -C. Chang , P. Chang , R. Cheaib , P. Cheema , V. Chekelian , B. G. Cheon , K. Chilikin , K. Chirapatpimol , H. -E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , S. Choudhury , L. Corona , L. M. Cremaldi , S. Das , F. Dattola , E. De La Cruz-Burelo , S. A. De La Motte , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , M. Destefanis , A. De Yta-Hernandez , R. Dhamija , A. Di Canto , F. Di Capua , J. Dingfelder , Z. Doležal , I. Domínguez Jiménez , T. V. Dong , M. Dorigo , K. Dort , S. Dreyer , S. Dubey , G. Dujany , P. Ecker , M. Eliachevitch , P. Feichtinger , T. Ferber , D. Ferlewicz , T. Fillinger , C. Finck , G. Finocchiaro , A. Fodor , F. Forti , A. Frey , B. G. Fulsom , A. Gabrielli , E. Ganiev , M. Garcia-Hernandez , G. Gaudino , V. Gaur , A. Gaz , A. Gellrich , G. Ghevondyan , D. Ghosh , G. Giakoustidis , R. Giordano , A. Giri , B. Gobbo , R. Godang , P. Goldenzweig , W. Gradl , T. Grammatico , S. Granderath , E. Graziani , D. Greenwald , Z. Gruberová , T. Gu , Y. Guan , K. Gudkova , S. Halder , Y. Han , T. Hara , K. Hayasaka , H. Hayashii , S. Hazra , C. Hearty , M. T. Hedges , I. Heredia de la Cruz , M. Hernández Villanueva , A. Hershenhorn , T. Higuchi , E. C. Hill , M. Hoek , M. Hohmann , C. -L. Hsu , T. Iijima , K. Inami , G. Inguglia , N. Ipsita , A. Ishikawa , S. Ito , R. Itoh , M. Iwasaki , P. Jackson , W. W. Jacobs , D. E. Jaffe , E. -J. Jang , Q. P. Ji , S. Jia , Y. Jin , A. Johnson , K. K. Joo , H. Junkerkalefeld , H. Kakuno , A. B. Kaliyar , J. Kandra , K. H. Kang , S. Kang , G. Karyan , T. Kawasaki , F. Keil , C. Ketter , C. Kiesling , C. -H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , T. Koga , S. Kohani , A. Korobov , S. Korpar , E. Kovalenko , R. Kowalewski , T. M. G. Kraetzschmar , P. Križan , P. Krokovny , M. Kumar , K. Kumara , T. Kunigo , A. Kuzmin , Y. -J. Kwon , S. Lacaprara , Y. -T. Lai , T. Lam , J. S. Lange , M. Laurenza , K. Lautenbach , R. Leboucher , F. R. Le Diberder , P. Leitl , D. Levit , C. Li , L. K. Li , J. Libby , Q. Y. Liu , Z. Q. Liu , S. Longo , A. Lozar , T. Lueck , C. Lyu , Y. Ma , M. Maggiora , R. Maiti , S. Maity , G. Mancinelli , R. Manfredi , E. Manoni , A. C. Manthei , M. Mantovano , D. Marcantonio , S. Marcello , C. Marinas , L. Martel , C. Martellini , A. Martini , T. Martinov , L. Massaccesi , M. Masuda , D. Matvienko , S. K. Maurya , J. A. McKenna , R. Mehta , F. Meier , M. Merola , F. Metzner , M. Milesi , C. Miller , M. Mirra , K. Miyabayashi , R. Mizuk , G. B. Mohanty , N. Molina-Gonzalez , S. Mondal , S. Moneta , H. -G. Moser , R. Mussa , I. Nakamura , Y. Nakazawa , A. Narimani Charan , M. Naruki , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , G. Nazaryan , M. Niiyama , N. K. Nisar , S. Nishida , S. Ogawa , H. Ono , Y. Onuki , P. Oskin , E. R. Oxford , P. Pakhlov , G. Pakhlova , A. Paladino , A. Panta , E. Paoloni , S. Pardi , K. Parham , H. Park , S. -H. Park , B. Paschen , S. Patra , S. Paul , T. K. Pedlar , R. Peschke , R. Pestotnik , M. Piccolo , L. E. Piilonen , P. L. M. Podesta-Lerma , T. Podobnik , S. Pokharel , L. Polat , C. Praz , S. Prell , E. Prencipe , M. T. Prim , H. Purwar , N. Rad , P. Rados , G. Raeuber , S. Raiz , M. Reif , S. Reiter , I. Ripp-Baudot , G. Rizzo , L. B. Rizzuto , S. H. Robertson , M. Roehrken , J. M. Roney , A. Rostomyan , N. Rout , D. A. Sanders , S. Sandilya , A. Sangal , L. Santelj , Y. Sato , V. Savinov , B. Scavino , M. Schnepf , C. Schwanda , Y. Seino , A. Selce , K. Senyo , J. Serrano , M. E. Sevior , C. Sfienti , W. Shan , C. Sharma , X. D. Shi , T. Shillington , J. -G. Shiu , D. Shtol , A. Sibidanov , F. Simon , J. B. Singh , J. Skorupa , R. J. Sobie , M. Sobotzik , A. Soffer , A. Sokolov , E. Solovieva , S. Spataro , B. Spruck , M. Starič , S. Stefkova , Z. S. Stottler , R. Stroili , M. Sumihama , W. Sutcliffe , H. Svidras , M. Takahashi , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , A. Thaller , O. Tittel , R. Tiwary , D. Tonelli , E. Torassa , K. Trabelsi , I. Tsaklidis , M. Uchida , I. Ueda , T. Uglov , K. Unger , Y. Unno , K. Uno , S. Uno , P. Urquijo , Y. Ushiroda , S. E. Vahsen , R. van Tonder , G. S. Varner , K. E. Varvell , A. Vinokurova , V. S. Vismaya , L. Vitale , V. Vobbilisetti , B. Wach , M. Wakai , H. M. Wakeling , S. Wallner , E. Wang , M. -Z. Wang , X. L. Wang , Z. Wang , A. Warburton , M. Watanabe , S. Watanuki , M. Welsch , C. Wessel , E. Won , X. P. Xu , B. D. Yabsley , S. Yamada , W. Yan , S. B. Yang , J. H. Yin , Y. M. Yook , K. Yoshihara , C. Z. Yuan , Y. Yusa , L. Zani , V. Zhilich , J. S. Zhou , Q. D. Zhou , V. I. Zhukova

We investigate the in-medium masses of the pseudoscalar $(D,{\bar D},D_s^{\pm})$, and vector $(D^*,\bar{D}^*, D_s^{*\pm})$, open charm mesons in isospin asymmetric magnetized nuclear matter, accounting for the effects of Dirac sea. The…

High Energy Physics - Phenomenology · Physics 2023-08-23 Sourodeep De , Pallabi Parui , Amruta Mishra

With the one-boson-exchange model we have studied the possible existence of the very loosely bound hidden-charm molecular baryons composed of anti-charmed meson and charmed baryon. Our numerical results indicate that there exist…

High Energy Physics - Phenomenology · Physics 2011-12-21 Zhong-Cheng Yang , Zhi-Feng Sun , Jun He , Xiang Liu , Shi-Lin Zhu

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

We report on a theoretical study of the hidden charm $N^*_{c \bar{c}}$ states in the $\gamma p \to \bar{D}^{*0} \Lambda^+_c$ reaction near threshold within an effective Lagrangian approach. In addition to the contributions from the…

Nuclear Theory · Physics 2017-01-04 Yin Huang , Ju-Jun Xie , Jun He , Xurong Chen , Hong-Fei Zhang

We report the first observation of a charm-strange meson DsJ(2632) at a mass of 2632.6+/-1.6 MeV/c^2 in data from SELEX, the charm hadro-production experiment E781 at Fermilab. This state is seen in two decay modes, Ds eta and D0 K+. In the…

High Energy Physics - Experiment · Physics 2010-04-06 The SELEX Collaboration , A. V. Evdokimov

The mass spectra of charm-strange mesons including ground, radial and orbital excitations have been calculated within a relativistic Dirac framework. The predicted masses of the ground state $1S$ and the first orbital excited state $1P$…

High Energy Physics - Phenomenology · Physics 2025-07-16 Bhoomika Pandya , Manan N Shah , P C Vinodkumar

A coupled-channel model previously employed to describe the narrow $D_{s0}^*$(2317) and broad $D_0^*$(2400) charmed scalar mesons is generalized so as to include all ground-state pseudoscalar-pseudoscalar and vector-vector two-meson…

High Energy Physics - Phenomenology · Physics 2008-11-26 Eef van Beveren , George Rupp

We study the properties of open-charm mesons ($D$ and $\bar {D}$) in nuclear matter at finite temperature within a self-consistent coupled-channel approach. The meson-baryon interactions are adopted from a type of broken SU(4) s-wave…

Nuclear Theory · Physics 2008-11-26 Laura Tolos , Angels Ramos , Tetsuro Mizutani

Motivated by the recent surprising discovery of two new meson states with c s-bar quark content but unexpectedly low masses and narrow total decay widths, we work out, in a nonrelativistic potential-model approach developed already some two…

High Energy Physics - Phenomenology · Physics 2009-11-10 Wolfgang Lucha , F. F. Schoberl

We present the recent results on charm baryon production and decays at Belle and Belle II experiments using a 1.4 ab$^{-1}$ data sample of $e^+ e^-$ collision collected at center-of-mass energies near the $\Upsilon(nS)$ resonances. The…

High Energy Physics - Experiment · Physics 2026-01-13 Alena Mufazalova

Considering abundant experimental information of charmed mesons and the present research status, in this work we systematically study higher radial and orbital excitations in the charmed meson family by analyzing the mass spectrum and…

High Energy Physics - Phenomenology · Physics 2015-10-09 Qin-Tao Song , Dian-Yong Chen , Xiang Liu , Takayuki Matsuki

We suggest that the recently observed charmed scalar mesons $D_0^{0}(2308)$ (BELLE) and $D_0^{0,+}(2405)$ (FOCUS) are considered as different resonances. Using the QCD sum rule approach we investigate the possible four-quark structure of…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. E. Bracco , A. Lozea , R. D. Matheus , F. S. Navarra , M. Nielsen

Identifying the t-channel exchange of vector mesons as the driving force for the s-wave scattering of pseudo-scalar mesons off the baryon ground states, a surprisingly rich spectrum of molecules is formed. We argue that chiral symmetry and…

High Energy Physics - Phenomenology · Physics 2010-12-16 J. Hofmann , M. F. M. Lutz

The effective theory for heavy quarks has additional symmetries with respect to QCD, which relate charm and beauty hadron masses. Assuming the spectrum of charmed particles, we predicted in a previous work the masses of some beauty…

High Energy Physics - Phenomenology · Physics 2015-06-25 Ugo Aglietti

We use overlap fermions as valence quarks to calculate meson masses in a wide quark mass range on the $2+1$-flavor domain-wall fermion gauge configurations generated by the RBC and UKQCD Collaborations. The well-defined quark masses in the…

The study of mesons and baryons which contain at least one charm quark is referred to as open charm physics. It offers the possibility to study up-type quark transitions. Since the $c$ quark can not be treated in any mass limit, theoretical…

High Energy Physics - Experiment · Physics 2017-06-06 Peter Weidenkaff

We study the properties of strange and charm mesons in hot and dense matter within a self-consistent coupled-channel approach for the experimental conditions of density and temperature expected for the CBM experiment at FAIR/GSI. The…

High Energy Physics - Phenomenology · Physics 2009-06-25 Laura Tolos , Daniel Cabrera , Daniel Gamermann , Tetsuro Mizutani , Raquel Molina , Eulogio Oset , Angels Ramos

The masses of heavy tetraquarks with hidden charm and bottom are calculated in the framework of the relativistic quark model. The tetraquark is considered as the bound state of a heavy-light diquark and antidiquark. The light quark in a…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. Ebert , R. N. Faustov , V. O. Galkin