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Related papers: J/psi Production at the LHC

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In this paper we study the $H + \gamma$ ($H = J/\Psi$ and $\Upsilon$) production in coherent hadron - hadron interactions at LHC energies. Considering the ultrarelativistic protons as a source of photons, we estimate the $\gamma + p…

High Energy Physics - Phenomenology · Physics 2015-06-05 V. P. Goncalves , M. M. Machado

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 consider the charmonium production in thermalized hadronic medium created in ultrarelativistic heavy ion collisions at LHC energy. The calculations for the secondary $J/\psi$ and $\psi^,$ production by $D\bar D$ annihilation are…

High Energy Physics - Phenomenology · Physics 2009-01-07 P. Braun-Munzinger , K. Redlich

For $J/\psi$ pair production at hadron colliders, we present the full next-to-leading order (NLO) calculations with the color-singlet channel in nonrelativistic QCD. We find that the NLO result can reasonably well describe the LHCb measured…

High Energy Physics - Phenomenology · Physics 2016-10-26 Li-Ping Sun , Hao Han , Kuang-Ta Chao

We briefly review recent results which we have obtained in the study of J/psi-pair production at the Tevatron and the LHC. We claim that the existing data set from CMS and D0 point at a significant double-parton-scattering contribution with…

High Energy Physics - Phenomenology · Physics 2016-11-08 Jean-Philippe Lansberg , Hua-Sheng Shao

The production rate of prompt $\psi'$'s at large transverse momentum at the Tevatron is larger than theoretical expectations by about a factor of 30. As a solution to this puzzle, we suggest that the dominant $\psi'$ production mechanism is…

High Energy Physics - Phenomenology · Physics 2016-08-24 Eric Braaten , Sean Fleming

Both hard and soft QCD dynamics are important in charmonium production, as presented here through a next-to-leading order QCD matrix element calculation combined with the colour evaporation model. Observed $x_F$ and $p_\perp$ distributions…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Brenner Mariotto , M. B. Gay Ducati , G. Ingelman

We study the process $\bar p p \rightarrow J/\psi + \gamma +X$ at the Tevatron energy ($\sqrt{s} = 1.8$~TeV). The perturbative QCD contributions to this process from the gluon-fusion and the fragmentation mechanisms are computed. For the…

High Energy Physics - Phenomenology · Physics 2009-10-28 D. P. Roy , K. Sridhar

Recent data from the Tevatron has revealed that the production rate of prompt charmonium at large transverse momentum is orders of magnitude larger than the best theoretical predictions of a few years ago. These surprising results can be…

High Energy Physics - Phenomenology · Physics 2009-10-28 E. Braaten , S. Fleming , T. C. Yuan

We calculate the partonic cross sections for the hadroproduction of polarized chi_{cJ} mesons using the factorization formalism of nonrelativistic QCD. We also describe how the polarization is passed on to the J/psi mesons in the radiative…

High Energy Physics - Phenomenology · Physics 2011-03-23 Bernd A. Kniehl , Jungil Lee

It has been proposed that the large cross sections for prompt $\psi$, $\psi'$, and $\chi_c$ production at the Fermilab Tevatron $p\bar p$ collider can be explained by a dominant color-octet term in the fragmentation function for a gluon to…

High Energy Physics - Phenomenology · Physics 2009-09-15 V. Barger , S. Fleming , R. J. N. Phillips

We investigate the pattern of asymmetries in the colour-octet model for inclusive production of charmonium with polarised initial state hadrons and photons. We find that singly polarised asymmetries vanish. The double polarised asymmetry…

High Energy Physics - Phenomenology · Physics 2009-10-28 Sourendu Gupta , Prakash Mathews

The polar and azimuthal angular distributions for the lepton pair arising from the decay of a J/psi meson produced at transverse momentum p_T balanced by a photon [or gluon] in hadronic collisions are calculated in the color singlet model…

High Energy Physics - Phenomenology · Physics 2009-10-28 C. S. Kim , E. Mirkes

We demonstrate that the recent studies of J/psi-pair production by CMS at the LHC and by D0 at the Tevatron reveal the presence of different production mechanisms in different kinematical regions. We find out that next-to-leading-order…

High Energy Physics - Phenomenology · Physics 2015-11-11 Jean-Philippe Lansberg , Hua-Sheng Shao

At existing and planned neutrino factories (high energy and high intensity neutrino beam facilities) precision studies of QCD in neutrino-nucleon interactions are a realistic opportunity. We investigate charmonium production in fixed target…

High Energy Physics - Phenomenology · Physics 2009-10-31 Alexey A. Petrov , Tibor Torma

The direct charmonium and bottomonium production rate observed at high-pt in pp-bar collisions at the Tevatron is factors of ten larger than predictions based on conventional perturbative QCD. We show that this excess can be accounted for…

High Energy Physics - Phenomenology · Physics 2009-10-30 A. Edin , G. Ingelman , J. Rathsman

With the recent LHCb data on $\eta_c$ production and based on heavy quark spin symmetry, we obtain the long-distance matrix elements for both $\eta_c$ and $J/\psi$ productions, among which, the color-singlet one for $\eta_c$ is obtained…

High Energy Physics - Phenomenology · Physics 2015-03-11 Hong-Fei Zhang , Zhan Sun , Wen-Long Sang , Rong Li

We report on forward-rapidity charmonium production in pp collisions at a center of mass energy $\sqrt{s} = 13$ TeV, as measured by ALICE at the LHC. Differential cross sections for both J/{\psi} and {\psi}(2S) are presented as a function…

Nuclear Experiment · Physics 2019-08-13 Pereira Da Costa Hugo

The production of J/psi mesons in proton-proton collisions at sqrt(s)=7 TeV is studied with the LHCb detector at the LHC. The differential cross-section for prompt J/psi production is measured as a function of the J/psi transverse momentum…

High Energy Physics - Experiment · Physics 2012-07-20 LHCb Collaboration , R. Aaij , B. Adeva , M. Adinolfi , C. Adrover , A. Affolder , Z. Ajaltouni , J. Albrecht , F. Alessio , M. Alexander , P. Alvarez Cartelle , A. A. Alves , S. Amato , Y. Amhis , J. Amoraal , J. Anderson , R. B. Appleby , O. Aquines Gutierrez , L. Arrabito , M. Artuso , E. Aslanides , G. Auriemma , S. Bachmann , D. S. Bailey , V. Balagura , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , A. Bates , C. Bauer , Th. Bauer , A. Bay , I. Bediaga , K. Belous , I. Belyaev , E. Ben-Haim , M. Benayoun , G. Bencivenni , R. Bernet , M. -O. Bettler , M. van Beuzekom , S. Bifani , A. Bizzeti , P. M. Bjørnstad , T. Blake , F. Blanc , C. Blanks , J. Blouw , S. Blusk , A. Bobrov , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , A. Borgia , E. Bos , T. J. V. Bowcock , C. Bozzi , T. Brambach , J. van den Brand , J. Bressieux , S. Brisbane , M. Britsch , T. Britton , N. H. Brook , H. Brown , A. Büchler-Germann , A. Bursche , J. Buytaert , S. Cadeddu , J. M. Caicedo Carvajal , O. Callot , M. Calvi , M. Calvo Gomez , A. Camboni , P. Campana , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , L. Carson , K. Carvalho Akiba , G. Casse , M. Cattaneo , M. Charles , Ph. Charpentier , N. Chiapolini , X. Cid Vidal , P. J. Clark , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , C. Coca , V. Coco , J. Cogan , P. Collins , F. Constantin , G. Conti , A. Contu , M. Coombes , G. Corti , G. A. Cowan , R. Currie , B. D'Almagne , C. D'Ambrosio , W. Da Silva , P. David , I. De Bonis , S. De Capua , M. De Cian , F. De Lorenzi , J. M. De Miranda , L. De Paula , P. De Simone , D. Decamp , H. Degaudenzi , M. Deissenroth , L. Del Buono , C. Deplano , O. Deschamps , F. Dettori , J. Dickens , H. Dijkstra , M. Dima , P. Diniz Batista , S. Donleavy , D. Dossett , A. Dovbnya , F. Dupertuis , R. Dzhelyadin , C. Eames , S. Easo , U. Egede , V. Egorychev , S. Eidelman , D. van Eijk , F. Eisele , S. Eisenhardt , L. Eklund , D. G. d'Enterria , D. Esperante Pereira , L. Estève , E. Fanchini , C. Färber , G. Fardell , C. Farinelli , S. Farry , V. Fave , V. Fernandez Albor , M. Ferro-Luzzi , S. Filippov , C. Fitzpatrick , F. Fontanelli , R. Forty , M. Frank , C. Frei , M. Frosini , J. L. Fungueirino Pazos , S. Furcas , A. Gallas Torreira , D. Galli , M. Gandelman , P. Gandini , Y. Gao , J-C. Garnier , J. Garofoli , L. Garrido , C. Gaspar , N. Gauvin , M. Gersabeck , T. Gershon , Ph. Ghez , V. Gibson , V. V. Gligorov , C. Göbel , D. Golubkov , A. Golutvin , A. Gomes , H. Gordon , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , G. Graziani , A. Grecu , S. Gregson , B. Gui , E. Gushchin , Yu. Guz , T. Gys , G. Haefeli , S. C. Haines , T. Hampson , S. Hansmann-Menzemer , R. Harji , N. Harnew , P. F. Harrison , J. He , K. Hennessy , P. Henrard , J. A. Hernando Morata , E. van Herwijnen , A. Hicheur , E. Hicks , W. Hofmann , K. Holubyev , P. Hopchev , W. Hulsbergen , P. Hunt , T. Huse , R. S. Huston , D. Hutchcroft , V. Iakovenko , C. Iglesias Escudero , P. Ilten , J. Imong , R. Jacobsson , M. Jahjah Hussein , E. Jans , F. Jansen , P. Jaton , B. Jean-Marie , F. Jing , M. John , D. Johnson , C. R. Jones , B. Jost , F. Kapusta , T. M. Karbach , J. Keaveney , U. Kerzel , T. Ketel , A. Keune , B. Khanji , Y. M. Kim , M. Knecht , S. Koblitz , A. Konoplyannikov , P. Koppenburg , A. Kozlinskiy , L. Kravchuk , G. Krocker , P. Krokovny , F. Kruse , K. Kruzelecki , M. Kucharczyk , S. Kukulak , R. Kumar , T. Kvaratskheliya , V. N. La Thi , D. Lacarrere , G. Lafferty , A. Lai , R. W. Lambert , G. Lanfranchi , C. Langenbruch , T. Latham , R. Le Gac , J. van Leerdam , J. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , O. Leroy , T. Lesiak , L. Li , Y. Y. Li , L. Li Gioi , M. Lieng , M. Liles , R. Lindner , C. Linn , B. Liu , G. Liu , J. H. Lopes , E. Lopez Asamar , N. Lopez-March , J. Luisier , B. M'charek , F. Machefert , I. V. Machikhiliyan , F. Maciuc , O. Maev , J. Magnin , A. Maier , S. Malde , R. M. D. Mamunur , G. Manca , G. Mancinelli , N. Mangiafave , U. Marconi , R. Märki , J. Marks , G. Martellotti , A. Martens , L. Martin , A. Martín Sánchez , D. Martinez Santos , A. Massafferri , Z. Mathe , C. Matteuzzi , M. Matveev , V. Matveev , E. Maurice , B. Maynard , A. Mazurov , G. McGregor , R. McNulty , C. Mclean , M. Meissner , M. Merk , J. Merkel , M. Merkin , R. Messi , S. Miglioranzi , D. A. Milanes , M. -N. Minard , S. Monteil , D. Moran , P. Morawski , J. V. Morris , R. Mountain , I. Mous , F. Muheim , K. Müller , R. Muresan , F. Murtas , B. Muryn , M. Musy , J. Mylroie-Smith , P. Naik , T. Nakada , R. Nandakumar , J. Nardulli , M. Nedos , M. Needham , N. Neufeld , M. Nicol , S. Nies , V. Niess , N. Nikitin , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , O. Okhrimenko , R. Oldeman , M. Orlandea , A. Ostankov , B. Pal , J. Palacios , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , C. 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Tuning , A. Ukleja , P. Urquijo , U. Uwer , V. Vagnoni , G. Valenti , R. Vazquez Gomez , P. Vazquez Regueiro , S. Vecchi , J. J. Velthuis , M. Veltri , K. Vervink , B. Viaud , I. Videau , X. Vilasis-Cardona , J. Visniakov , A. Vollhardt , D. Voong , A. Vorobyev , An. Vorobyev , H. Voss , K. Wacker , S. Wandernoth , J. Wang , D. R. Ward , A. D. Webber , D. Websdale , M. Whitehead , D. Wiedner , L. Wiggers , G. Wilkinson , M. P. Williams , M. Williams , F. F. Wilson , J. Wishahi , M. Witek , W. Witzeling , S. A. Wotton , K. Wyllie , Y. Xie , F. Xing , Z. Yang , G. Ybeles Smit , R. Young , O. Yushchenko , M. Zavertyaev , L. Zhang , W. C. Zhang , Y. Zhang , A. Zhelezov , L. Zhong , E. Zverev

We briefly review the existing psi(2S) data taken at RHIC, the Tevatron and the LHC. We systematically compare them with colour-singlet-model predictions as a function of the center-of-mass energy, of the quarkonium rapidity and of the…

High Energy Physics - Phenomenology · Physics 2013-03-13 J. P. Lansberg
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