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Related papers: Prospects for X(3872) Detection at Panda

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We discuss methods and approaches to the description of molecular states in the spectrum of heavy quarks and investigate in detail various properties of the exotic charmonium-like state X(3872) in the framework of the mesonic molecule…

High Energy Physics - Phenomenology · Physics 2019-08-30 Yu. S. Kalashnikova , A. V. Nefediev

In order to understand the structure of the X(3872), the $c \bar c$ charmonium core state coupling to the $D^0 \bar D^{\ast 0}$ and $D^+ D^{\ast -}$ molecular states are studied. The strengths of the couplings between the charmonium state…

High Energy Physics - Phenomenology · Physics 2014-05-07 Makoto Takizawa , Sachiko Takeuchi

The observation of many unexpected states decaying into heavy quarkonia has challenged the usual Q-Qbar interpretation. We will discuss the nature of some of the charmonium-like resonances recently observed by BES III and LHCb, and their…

High Energy Physics - Phenomenology · Physics 2016-09-21 A. Pilloni

We study the radiative decay of $X(3872)$ based on the assumption that $X(3872)$ is regarded as a $c\overline{c}$ charmonium with quantum number $J^{PC}=1^{++}$ ($J,\,P,\,C$ represent the spin, parity and charge conjugation, respectively).…

High Energy Physics - Phenomenology · Physics 2023-12-25 Shuo-Ying Yu , Xian-Wei Kang

We study the X(3872)-->D^0 \bar D^0 \pi^0 decay within a D \bar D^* molecular picture for the X(3872) state. This decay mode is more sensitive to the long-distance structure of the X(3872) resonance than its J/\psi\pi\pi and J/\psi3\pi…

High Energy Physics - Phenomenology · Physics 2014-06-02 Feng-Kun Guo , Carlos Hidalgo-Duque , Juan Nieves , Altug Ozpineci , Manuel Pavon Valderrama

The exclusive charmonium production process in $\bar{p}p$ annihilation with an associated $\pi^0$ meson $\bar{p}p\to J/\psi\pi^0$ is studied in the framework of QCD collinear factorization. The feasibility of measuring this reaction through…

Nuclear Experiment · Physics 2017-02-22 PANDA Collaboration , B. Singh , W. Erni , B. Krusche , M. Steinacher , N. Walford , H. Liu , Z. Liu , B. Liu , X. Shen , C. Wang , J. Zhao , M. Albrecht , T. Erlen , M. Fink , F. H. Heinsius , T. Held , T. Holtmann , S. Jasper , I. Keshk , H. Koch , B. Kopf , M. Kuhlmann , M. Kümmel , S. Leiber , M. Mikirtychyants , P. Musiol , A. Mustafa , M. Pelizäus , J. Pychy , M. Richter , C. Schnier , T. Schröder , C. Sowa , M. Steinke , T. Triffterer , U. Wiedner , M. Ball , R. Beck , C. Hammann , B. Ketzer , M. Kube , P. Mahlberg , M. Rossbach , C. Schmidt , R. Schmitz , U. Thoma , M. Urban , D. Walther , C. Wendel , A. Wilson , A. Bianconi , M. Bragadireanu , M. Caprini , D. Pantea , B. Patel , W. Czyzycki , M. Domagala , G. Filo , J. Jaworowski , M. Krawczyk , E. Lisowski , F. Lisowski , M. Michałek , P. Poznański , J. Płażek , K. Korcyl , A. Kozela , P. Kulessa , P. Lebiedowicz , K. Pysz , W. Schäfer , A. Szczurek , T. Fiutowski , M. Idzik , B. Mindur , D. Przyborowski , K. Swientek , J. Biernat , B. Kamys , S. Kistryn , G. Korcyl , W. Krzemien , A. Magiera , P. Moskal , A. Pyszniak , Z. Rudy , P. Salabura , J. Smyrski , P. Strzempek , A. Wronska , I. Augustin , R. Böhm , I. Lehmann , D. Nicmorus Marinescu , L. Schmitt , V. Varentsov , M. Al-Turany , A. Belias , H. Deppe , N. Divani Veis , R. Dzhygadlo , A. Ehret , H. Flemming , A. Gerhardt , K. Götzen , A. Gromliuk , L. Gruber , R. Karabowicz , R. Kliemt , M. Krebs , U. Kurilla , D. Lehmann , S. Löchner , J. Lühning , U. Lynen , H. Orth , M. Patsyuk , K. Peters , T. Saito , G. Schepers , C. J. Schmidt , C. Schwarz , J. Schwiening , A. Täschner , M. Traxler , C. Ugur , B. Voss , P. Wieczorek , A. Wilms , M. Zühlsdorf , V. Abazov , G. Alexeev , V. A. Arefiev , V. Astakhov , M. Yu. Barabanov , B. V. Batyunya , Y. Davydov , V. Kh. Dodokhov , A. Efremov , A. Fechtchenko , A. G. Fedunov , A. Galoyan , S. Grigoryan , E. K. Koshurnikov , Y. Yu. Lobanov , V. I. Lobanov , A. F. Makarov , L. V. Malinina , V. Malyshev , A. G. Olshevskiy , E. Perevalova , A. A. Piskun , T. Pocheptsov , G. Pontecorvo , V. Rodionov , Y. Rogov , R. Salmin , A. Samartsev , M. G. Sapozhnikov , G. Shabratova , N. B. Skachkov , A. N. Skachkova , E. A. Strokovsky , M. Suleimanov , R. Teshev , V. Tokmenin , V. Uzhinsky , A. Vodopianov , S. A. Zaporozhets , N. I. Zhuravlev , A. Zinchenko , A. G. Zorin , D. Branford , D. Glazier , D. Watts , M. Böhm , A. Britting , W. Eyrich , A. Lehmann , M. Pfaffinger , F. Uhlig , S. Dobbs , K. Seth , A. Tomaradze , T. Xiao , D. Bettoni , V. Carassiti , A. Cotta Ramusino , P. Dalpiaz , A. Drago , E. Fioravanti , I. Garzia , M. Savrie , V. Akishina , I. Kisel , G. Kozlov , M. Pugach , M. Zyzak , P. Gianotti , C. Guaraldo , V. Lucherini , A. Bersani , G. Bracco , M. Macri , R. F. Parodi , K. Biguenko , K. T. Brinkmann , V. Di Pietro , S. Diehl , V. Dormenev , P. Drexler , M. Düren , E. Etzelmüller , M. Galuska , E. Gutz , C. Hahn , A. Hayrapetyan , M. Kesselkaul , W. Kühn , T. Kuske , J. S. Lange , Y. Liang , V. Metag , M. Moritz , M. Nanova , S. Nazarenko , R. Novotny , T. Quagli , S. Reiter , A. Riccardi , J. Rieke , C. Rosenbaum , M. Schmidt , R. Schnell , H. Stenzel , U. Thöring , T. Ullrich , M. N. Wagner , T. Wasem , B. Wohlfahrt , H. G. Zaunick , E. Tomasi-Gustafsson , D. Ireland , G. Rosner , B. Seitz , P. N. Deepak , A. Kulkarni , A. Apostolou , M. Babai , M. Kavatsyuk , P. J. Lemmens , M. Lindemulder , H. Loehner , J. Messchendorp , P. Schakel , H. Smit , M. Tiemens , J. C. van der Weele , R. Veenstra , S. Vejdani , K. Dutta , K. Kalita , A. Kumar , A. Roy , H. Sohlbach , M. Bai , L. Bianchi , M. Büscher , L. Cao , A. Cebulla , R. Dosdall , A. Gillitzer , F. Goldenbaum , D. Grunwald , A. Herten , Q. Hu , G. Kemmerling , H. Kleines , A. Lai , A. Lehrach , R. Nellen , H. Ohm , S. Orfanitski , D. Prasuhn , E. Prencipe , J. Pütz , J. Ritman , S. Schadmand , T. Sefzick , V. Serdyuk , G. Sterzenbach , T. Stockmanns , P. Wintz , P. Wüstner , H. Xu , A. Zambanini , S. Li , Z. Li , Z. Sun , H. Xu , V. Rigato , L. Isaksson , P. Achenbach , O. Corell , A. Denig , M. Distler , M. Hoek , A. Karavdina , W. Lauth , Z. Liu , H. Merkel , U. Müller , J. Pochodzalla , S. Sanchez , S. Schlimme , C. Sfienti , M. Thiel , H. Ahmadi , S. Ahmed , S. Bleser , L. Capozza , M. Cardinali , A. Dbeyssi , M. Deiseroth , F. Feldbauer , M. Fritsch , B. Fröhlich , D. Kang , D. Khaneft , R. Klasen , H. H. Leithoff , D. Lin , F. Maas , S. Maldaner , M. Martínez , M. Michel , M. C. Mora Espí , C. Morales Morales , C. Motzko , F. Nerling , O. Noll , S. Pflüger , A. Pitka , D. Rodríguez Piñeiro , A. Sanchez-Lorente , M. Steinen , R. Valente , T. Weber , M. Zambrana , I. Zimmermann , A. Fedorov , M. Korjik , O. Missevitch , A. Boukharov , O. Malyshev , I. Marishev , V. Balanutsa , P. Balanutsa , V. Chernetsky , A. Demekhin , A. Dolgolenko , P. Fedorets , A. Gerasimov , V. Goryachev , V. Chandratre , V. Datar , D. Dutta , V. Jha , H. Kumawat , A. K. Mohanty , A. Parmar , B. Roy , G. Sonika , C. Fritzsch , S. Grieser , A. K. Hergemöller , B. Hetz , N. Hüsken , A. Khoukaz , J. P. Wessels , K. Khosonthongkee , C. Kobdaj , A. Limphirat , P. Srisawad , Y. Yan , A. Yu. Barnyakov , M. Barnyakov , K. Beloborodov , V. E. Blinov , V. S. Bobrovnikov , I. A. Kuyanov , K. Martin , A. P. Onuchin , S. Serednyakov , A. Sokolov , Y. Tikhonov , A. E. Blinov , S. Kononov , E. A. Kravchenko , E. Atomssa , R. Kunne , B. Ma , D. Marchand , B. Ramstein , J. van de Wiele , Y. Wang , G. Boca , S. Costanza , P. Genova , P. Montagna , A. Rotondi , V. Abramov , N. Belikov , S. Bukreeva , A. Davidenko , A. Derevschikov , Y. Goncharenko , V. Grishin , V. Kachanov , V. Kormilitsin , A. Levin , Y. Melnik , N. Minaev , V. Mochalov , D. Morozov , L. Nogach , S. Poslavskiy , A. Ryazantsev , S. Ryzhikov , P. Semenov , I. Shein , A. Uzunian , A. Vasiliev , A. Yakutin , U. Roy , B. Yabsley , S. Belostotski , G. Gavrilov , A. Izotov , S. Manaenkov , O. Miklukho , D. Veretennikov , A. Zhdanov , T. Bäck , B. Cederwall , K. Makonyi , M. Preston , P. E. Tegner , D. Wölbing , A. K. Rai , S. Godre , D. Calvo , S. Coli , P. De Remigis , A. Filippi , G. Giraudo , S. Lusso , G. Mazza , M. Mignone , A. Rivetti , R. Wheadon , A. Amoroso , M. P. Bussa , L. Busso , F. De Mori , M. Destefanis , L. Fava , L. Ferrero , M. Greco , J. Hu , L. Lavezzi , M. Maggiora , G. Maniscalco , S. Marcello , S. Sosio , S. Spataro , F. Balestra , F. Iazzi , R. Introzzi , A. Lavagno , J. Olave , R. Birsa , F. Bradamante , A. Bressan , A. Martin , H. Calen , W. Ikegami Andersson , T. Johansson , A. Kupsc , P. Marciniewski , M. Papenbrock , J. Pettersson , K. Schönning , M. Wolke , B. Galnander , J. Diaz , V. Pothodi Chackara , A. Chlopik , G. Kesik , D. Melnychuk , B. Slowinski , A. Trzcinski , M. Wojciechowski , S. Wronka , B. Zwieglinski , P. Bühler , J. Marton , D. Steinschaden , K. Suzuki , E. Widmann , J. Zmeskal , K. M. Semenov-Tian-Shansky

In recent years the B-factories and other machines have found evidence for a large number of new states with hidden charm: candidate h_c(1P), eta_c(2S), and chi_{c2}(2P) states; the well-established X(3872); enhancements called X(3940),…

High Energy Physics - Experiment · Physics 2008-11-26 B. D. Yabsley

A candidate for the charmonium(like) state X(3872) is found 11 +/- 7 MeV below the DD* threshold using dynamical Nf=2 lattice simulation with J^PC=1^++ and I=0. This is the first lattice simulation that establishes a candidate for X(3872)…

High Energy Physics - Lattice · Physics 2014-04-17 Sasa Prelovsek , Luka Leskovec

Two decades after its unexpected discovery, the properties of the $X(3872)$ exotic resonance are still under intense scrutiny. In particular, there are doubts about its nature as an ensemble of mesons or having any other internal structure.…

High Energy Physics - Phenomenology · Physics 2021-10-04 M. C. Gordillo , F. De Soto , J. Segovia

The Anti-Proton ANnihilation at DArmstadt (PANDA) experiment proposed at the Facility for Antiproton and Ion Research (FAIR) in Darmstadt (Germany) will perform a high precision spectroscopy of charmonium and exotic hadrons, such as…

Computational Physics · Physics 2019-08-13 Aleksandra Biegun

We study the production of $Z^\pm(4430)$ at a nucleon-antinucleon scattering experiment. Considering the PANDA experiment to be an ideal platform to explore the production of the charmonium and charmonim-like states, we suggest the…

High Energy Physics - Phenomenology · Physics 2008-11-27 Hong-Wei Ke , Xiang Liu

Monte Carlo simulations are powerful tools for understanding the effects of radiation interactions within detector devices allowing not only to evaluate typical estimates for experimental measurements and to serve as means for designing…

Instrumentation and Detectors · Physics 2016-02-09 F. Marinho , K. Akiba

A brief review of experimental results on charmonium and charmonium-like hadron spectroscopy at B-factories is presented. A special focus is put on recent results of eta_c and eta_c(2S) study, X(3872) radiative decays, omega J/psi final…

High Energy Physics - Experiment · Physics 2019-08-13 Dmitri Liventsev

Starting from a molecular picture for the X(3872) resonance, this state and its J^{PC}=2++ HQSS partner [X2(4012)] are analyzed within a model which incorporates possible mixings with 2P charmonium states. Since it is reasonable to expect…

High Energy Physics - Phenomenology · Physics 2016-11-23 E. Cincioglu , J. Nieves , A. Ozpineci , A. U. Yilmazer

The recent results on charmonium and charmoniumlike states from Belle experiment are reviewed. We summarise searches in $B$ decays for possible $X$-like states in final states containing $\eta_c$. The new measurement of…

High Energy Physics - Experiment · Physics 2015-09-15 Xiaolong Wang

We construct line shapes for the X(3872) that generalize the Flatte and zero-range line shapes that have been considered previously. These line shapes are associated with scattering amplitudes that are exactly unitary for real values of the…

High Energy Physics - Phenomenology · Physics 2015-03-17 Pierre Artoisenet , Eric Braaten , Daekyoung Kang

The charmonium spectrum is calculated with two nonrelativistic quark models, the linear potential model and the screened potential model. Using the obtained wavefunctions, we evaluate the electromagnetic transitions of charmonium states up…

High Energy Physics - Phenomenology · Physics 2017-03-01 Wei-Jun Deng , Hui Liu , Long-Cheng Gui , Xian-Hui Zhong

The recent results on Charmonium and Charmonium-like states at BESIII are reviewed, including the observation of $\rm Z_{cs}(3985)$ state, the study of the new decay modes of $\psi_2(3823)$ state, observation of resonance structure in $\rm…

High Energy Physics - Experiment · Physics 2022-12-15 Weimin Song

Assuming that $X(3872)$ is a mixture between $2P$ charmonium and $\bar{D}D^{*}$ molecular states with $J^{PC}=1^{++}$, an analysis of $X(3872)$ radiative decays into $J/\psi \gamma$ and $\psi(2S)\gamma$ is presented. The modification of the…

High Energy Physics - Phenomenology · Physics 2019-08-21 E. Cincioglu , A. Ozpineci

The B factories provide a unique playground for studying the properties of conventional and exotic charmonium states. We present recent results in initial state radiation and two-photon fusion, obtained using the full data set collected by…

High Energy Physics - Experiment · Physics 2013-11-06 Denis Bernard