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Related papers: Associated Charmonium Production in Low Energy p-p…

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In this paper we summarize our recent results for low energy associated charmonium production cross sections, using 1) crossing symmetry, and 2) an explicit hadronic model. These predictions are of relevance to the planned charmonium and…

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

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

We propose to investigate various charmonium states using their common decay channel to p pbar at LHC. Having the branching ratios for charmonium decaying into the p pbar final state measured or calculated, we propose to measure the…

High Energy Physics - Phenomenology · Physics 2013-05-30 Sergey Barsuk , Jibo He , Emi Kou , Benoit Viaud

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 this work, we calculate the total cross sections and the center-of-mass frame angular distributions of the charmonium production plus a light meson by the low energy $p\bar{p}$ interaction. The results of $p\bar{p}\to \pi^0 \Psi$ with…

High Energy Physics - Phenomenology · Physics 2012-08-08 Qing-Yong Lin , Xiang Liu , Hu-Shan Xu

The J/\Psi(1S) and \Psi'(2S) production near threshold in antiproton-nucleus reactions is calculated on the basis of the Glauber model. The model takes into account the antiproton (pre)absorption, proton Fermi motion, and charmonium…

Nuclear Theory · Physics 2013-05-22 A. B. Larionov , M. Bleicher , A. Gillitzer , M. Strikman

The study of the charmonium (cbar c) system is a powerful tool to understand the strong interaction. In pbar p annihilations studied with PANDA, the mass and width of the charmonium state, such as h_c, will be measured with an excellent…

Data Analysis, Statistics and Probability · Physics 2019-08-13 Aleksandra Biegun

We study the baryonic charmonium decays of $B$ mesons, $B^+ \to \eta_c K^+$ and $B^+ \to J/\psi K^+$, where $\eta_c$ and $J/\psi$ subsequently decay into a $p\bar p$ or $\Lambda\bar\Lambda$ pair. The charmonium produced in the above $B$…

High Energy Physics - Experiment · Physics 2019-08-14 K. Abe

Charmonium production and suppression in heavy-ion collisions at relativistic energies is investigated within different models, i.e. the comover absorption model, the threshold suppression model, the statistical coalescence model and the…

Nuclear Theory · Physics 2009-11-10 E. L. Bratkovskaya , A. P. Kostyuk , W. Cassing , H. Stoecker

Massless perturbative QCD forbids, at leading order, the exclusive annihilation of proton-antiproton into some charmonium states, which, however, have been observed in the $p\bar p$ channel, indicating the significance of higher order and…

High Energy Physics - Phenomenology · Physics 2009-10-28 M. Anselmino , F. Caruso , F. Murgia , M. R. Negrao

We consider the production of charmonium by $D\bar D$ annihilation during the mixed and hadronic phase of Pb-Pb collision at LHC energy. The calculations for secondary $J/\psi$ and $\psi^,$ production are performed within a kinetic model…

Nuclear Theory · Physics 2015-06-26 P. Braun-Munzinger , K. Redlich

We discuss the production of charmonium states in antiproton-nucleus collisions at the $\psi'$ threshold. It is explained that measurements in $\bar p A$ collisions will allow to get new information about the strengths of the inelastic…

Nuclear Theory · Physics 2015-06-26 L. Gerland

Studies of charmonium properties and production mechanism started with the discovery of $J/\psi$ meson. Since more than 40 years the charmonium production mechanism is still not entirely understood. Following the era of investigations at…

High Energy Physics - Experiment · Physics 2019-10-22 Andrii Usachov

We study the structures in cross sections and R ratios concerning electron-positron annihilation reactions, for open-strangeness, open-charm and open-beauty hadron-pair production, from the perspective of a recently developed production…

High Energy Physics - Phenomenology · Physics 2009-11-19 Eef van Beveren , George Rupp

The ALICE Collaboration at the LHC has measured the J/$\psi$ and $\psi^{'}$ photoproduction at mid-rapidity in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV. The charmonium is identified via its leptonic decay for events…

Nuclear Experiment · Physics 2014-11-10 ALICE Collaboration

The couplings of charmonia and charmonium hybrids (generically Psi) to ppbar are of great interest in view of future plans to study these states using an antiproton storage ring at GSI. These low to moderate energy Psi-ppbar couplings are…

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

Using 22.7 million BBbar events recorded with the BABAR detector, the inclusive branching fractions for the production of J/psi, psi(2S) and Chi_c in B decays are presented. Combining the charmonium state with a K+-, K0, K*+-, K*0 or…

High Energy Physics - Experiment · Physics 2007-05-23 G. Calderini

Using information on B-meson fragmentation functions from CERN LEP 1 and adopting the nonrelativistic QCD factorization formalism proposed by Bodwin, Braaten, and Lepage, we predict the transverse-momentum distribution of J/psi mesons…

High Energy Physics - Phenomenology · Physics 2011-03-23 B. A. Kniehl , G. Kramer

We study the production of the exotic charged charmonium-like state $Z_c^{\pm}(3900)$ in $p \bar p$ collisions through the sequential process $\psi(4260) \rightarrow Z_c^{\pm}(3900) \pi^{\mp}$, $Z_c^{\pm}(3900) \rightarrow J/\psi…

High Energy Physics - Experiment · Physics 2019-09-09 D0 Collaboration

Annihilation dynamics plays a fundamental role in the baryon$-$antibaryon interaction (B$-\rm{\overline{B}}$) at low-energy and its strength and range are crucial in the assessment of possible baryonic bound states. Experimental data on…

Nuclear Experiment · Physics 2022-12-12 ALICE Collaboration
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