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Related papers: Charm Physics Performance Studies for PANDA

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The QCD mechanisms underlying the exclusive strong decays and hadronic production amplitudes of charmonium remain poorly understood, despite decades of study and an increasingly detaled body of experimental information. One set of hadronic…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Barnes , X. Li

The elaborate analysis of spectrum of charmonium states and charmed hybrids in the mass region over DD-threshold is given. The combined approach based on the potential model and relativistic spherical symmetric top model for decay products…

High Energy Physics - Phenomenology · Physics 2011-08-31 M. Yu. Barabanov , A. S. Vodopyanov , V. Kh. Dodokhov , V. A. Babkin

We examine the invariant mass spectrum of $D^{0}p$ in $\bar B^0\to p\bar p D^{0}$ decay measured by BABAR and find that through the 2-step processes of $\bar B^0\to {\bf B_c^+}(\to D^{0} p)\bar p$, where ${\bf B_c}$ denotes a charmed baryon…

High Energy Physics - Phenomenology · Physics 2014-02-07 Hai-Yang Cheng , C. Q. Geng , Y. K. Hsiao

While experiment produced a candidate for the 1^P_1 chamonium in the past, it still requires a confirmation. Given the recent progress in the exclusive B decay into charmonia, we now have an opportunity to detect this charmonium (h_c) by…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. Suzuki

Physics with antiprotons in the charmonium mass region will play a major role at the future PANDA experiment at the FAIR facility in Darmstadt. At PANDA, an antiproton beam with momenta up to 15 GeV/c circulating in the high-energy storage…

Instrumentation and Detectors · Physics 2013-12-18 Kai-Thomas Brinkmann

The cross sections for the charmonium production processes p pbar -> m Psi, where m is a light meson and Psi is a charmonium state, are of great interest for the planned p-pbar experiment PANDA. In this paper we estimate these cross…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Lundborg , T. Barnes , U. Wiedner

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

The PANDA detector at FAIR aims to conduct an antiproton-proton experiment with a very high rate capability. It is expected to feature high mass resolution, more than 20 times better than achieved at B-factories. PANDA is in a unique…

High Energy Physics - Experiment · Physics 2015-10-13 Elisabetta Prencipe

In this talk, I review the recent experimental results on charmonium spectroscopy from BESIII, Belle, BaBar and CLEOc. Below the open-charm threshold, the masses and widths of spin-singlet states eta_c, eta_c(2S), h_c are measured with high…

High Energy Physics - Experiment · Physics 2013-11-15 Jingzhi Zhang

We review the most recent results from experiments studying systems containing charmed quarks. The selection reflects the presenter's bias, and there is an emphasis on decays of open charm. We discuss precision measurements of various…

High Energy Physics - Experiment · Physics 2007-05-23 Jim Napolitano

The exploration of symmetry laws stands as a cutting-edge direction in modern physics research. This work delves into the examination of P and CP symmetry properties within the charm quark system by analyzing asymmetry parameters in the…

High Energy Physics - Phenomenology · Physics 2026-04-21 Yunlu Wang , Yunlong Xiao , Pengcheng Hong

New results from charm experiments have led to renewed interest in this physics. The charm sector is now seen as a powerful tool to search for new physics and to advance our understanding of the standard model. We owe much of this progress…

High Energy Physics - Experiment · Physics 2014-11-17 Alex Smith

In this invited talk I discuss two recent applications of charmonium (Psi) decays to N Nbar m final states, where N is a nucleon and m is a light meson. There are several motivations for studying these decays: 1) They are useful for the…

High Energy Physics - Phenomenology · Physics 2015-05-20 T. Barnes

Charm and charmonium physics have gained renewed interest in the past decade. Recent spectroscopic observations strongly motivate these studies. Among the several possible reactions, measurements in proton-antiproton annihilation play an…

High Energy Physics - Experiment · Physics 2016-06-22 Elisabetta Prencipe , Jens Soeren Lange , Alexander Blinov

In this work, we calculate the charmonium spectrum and strong decay widths of cc states. The calculations are performed using the quark potential model with which incorporates the relativistic effects. The resulting cc spectrum exhibits a…

High Energy Physics - Phenomenology · Physics 2025-04-11 Zaki Ahmad , Ishrat Asghar , Faisal Akram , Bilal Masud

In this paper, we discuss the theoretical framework and the experimental measurements of the magnetic moment of the charm baryons. The $\Lambda_c^+$ magnetic moment is particularly interesting since it is equal to the magnetic moment of the…

High Energy Physics - Phenomenology · Physics 2020-05-20 A. S. Fomin , S. Barsuk , A. Yu. Korchin , V. A. Kovalchuk , E. Kou , M. Liul , A. Natochii , E. Niel , P. Robbe , A. Stocchi

We revise and extend expectations for the properties of charmonium states that lie above charm threshold, in light of new experimental information. We refine the Cornell coupled-channel model for the coupling of c-cbar levels to two-meson…

High Energy Physics - Phenomenology · Physics 2014-11-18 Estia J. Eichten , Kenneth Lane , Chris Quigg

In this talk, we review the recent experimental developments on charmonium and charm spectroscopy base on the data samples taken by the BESIII, Belle, LHCb and CMS experiments. We concentrate on the resonant parameter measurement of…

High Energy Physics - Experiment · Physics 2019-06-24 Y. Hu

A recent combination of measurements performed by the LHCb collaboration determined that $\gamma=(63.8^{+3.5}_{-3.7})^\circ$. The fit combined the results of $\gamma$ and charm measurements, which resulted in precision improvements for the…

High Energy Physics - Experiment · Physics 2024-04-30 Innes Mackay

The study of the $B^{+}\to p \bar p K^{+}$ decay channel at LHCb offers great opportunities to study different aspects of the Standard Model and possibly Beyond Standard Model physics. In particular it can be interesting not only for the…

High Energy Physics - Experiment · Physics 2019-08-13 R. Cardinale
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