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Related papers: Cross sections for 2-to-1 meson-meson scattering

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Collisional processes in ultrarelativistic N=1 SUSY QED plasma are studied and compared to those in an electromagnetic plasma of electrons, positrons and photons. Cross sections of all binary interactions which occur in the supersymmetric…

High Energy Physics - Theory · Physics 2015-03-19 Alina Czajka , Stanislaw Mrowczynski

We have measured the differential cross section for the inclusive production of psi(2S) mesons decaying to mu^{+} mu^{-1} that were produced in prompt or B-decay processes from ppbar collisions at 1.96 TeV. These measurements have been made…

High Energy Physics - Experiment · Physics 2009-08-26 CDF Collaboration , T. Aaltonen

We consider the process gamma^* N -> M_1 M_2 N' with a large rapidity gap between the two mesons M_1 and M_2. Within the QCD collinear approximation, the scattering amplitude may be written as a convolution of an impact factor describing…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Yu. Ivanov , B. Pire , L. Szymanowski , O. V. Teryaev

Two-quark--two-antiquark systems with four different quark flavors are considered in the framework of two-dimensional QCD, in the light-cone gauge, at leading orders of the $1/N_c^{}$ expansion. Introducing basis functions with…

High Energy Physics - Phenomenology · Physics 2025-09-22 Hagop Sazdjian

The differential cross-section for the inclusive production of psi(2S) mesons in pp collisions at sqrt(s)=7 TeV has been measured with the LHCb detector. The data sample corresponds to an integrated luminosity of 36 pb-1. The psi(2S) mesons…

High Energy Physics - Experiment · Physics 2020-07-28 LHCb collaboration , R. Aaij , C. Abellán Beteta , B. Adeva , M. Adinolfi , C. Adrover , A. Affolder , Z. Ajaltouni , J. Albrecht , F. Alessio , M. Alexander , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , Y. Amhis , J. Anderson , F. Andrianala , R. B. Appleby , F. Archilli , L. Arrabito , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , S. Bachmann , J. J. Back , D. S. Bailey , V. Balagura , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , A. Bates , Th. Bauer , A. Bay , I. Bediaga , S. Belogurov , K. Belous , I. Belyaev , E. Ben-Haim , M. Benayoun , G. Bencivenni , S. Benson , J. Benton , R. Bernet , M. O. Bettler , M. van Beuzekom , A. Bien , 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 , T. J. V. Bowcock , C. Bozzi , T. Brambach , J. van den Brand , J. Bressieux , D. Brett , M. Britsch , T. Britton , N. H. Brook , H. Brown , A. Bursche , J. Buytaert , A. Büchler-Germann , S. Cadeddu , 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 , Ch. Cauet , M. Charles , Ph. Charpentier , N. Chiapolini , M. Chrzaszcz , P. Ciambrone , K. Ciba , X. Cid Vidal , G. Ciezarek , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , C. Coca , V. Coco , J. Cogan , P. Collins , A. Comerma-Montells , F. Constantin , A. Cook , M. Coombes , G. Corti , B. Couturier , G. A. Cowan , R. Currie , C. D'Ambrosio , P. David , P. N. Y. David , O. De Aguiar Francisco , K. De Bruyn , M. De Cian , F. De Lorenzi , J. M. De Miranda , L. De Paula , P. De Simone , D. Decamp , M. Deckenhoff , H. Degaudenzi , L. Del Buono , C. Deplano , D. Derkach , O. Deschamps , F. Dettori , J. Dickens , H. Dijkstra , P. Diniz Batista , F. Domingo Bonal , S. Donleavy , F. Dordei , A. Dosil Suárez , D. Dossett , A. Dovbnya , F. Dupertuis , R. Dzhelyadin , A. Dziurda , S. Easo , U. Egede , V. Egorychev , S. Eidelman , D. van Eijk , F. Eisele , S. Eisenhardt , R. Ekelhof , L. Eklund , Ch. Elsasser , D. Elsby , D. Esperante Pereira , A. Falabella , E. Fanchini , G. Fardell , C. Farinelli , S. Farry , V. Fave , V. Fernandez Albor , F. Ferreira Rodrigues , M. Ferro-Luzzi , S. Filippov , C. Fitzpatrick , M. Fontana , F. Fontanelli , R. Forty , M. Frank , C. Frei , M. Frosini , S. Furcas , C. Färber , A. Gallas Torreira , D. Galli , M. Gandelman , P. Gandini , Y. Gao , J-C. Garnier , J. Garofoli , J. Garra Tico , L. Garrido , D. Gascon , C. Gaspar , R. Gauld , N. Gauvin , M. Gersabeck , T. Gershon , Ph. Ghez , V. Gibson , V. V. Gligorov , D. Golubkov , A. Golutvin , A. Gomes , H. Gordon , C. Gotti , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , G. Graziani , A. Grecu , E. Greening , S. Gregson , B. Gui , E. Gushchin , Yu. Guz , T. Gys , C. Göbel , C. Hadjivasiliou , G. Haefeli , C. Haen , S. C. Haines , T. Hampson , S. Hansmann-Menzemer , R. Harji , N. Harnew , J. Harrison , P. F. Harrison , T. Hartmann , J. He , V. Heijne , K. Hennessy , P. Henrard , J. A. Hernando Morata , E. van Herwijnen , E. Hicks , K. Holubyev , W. Hulsbergen , P. Hunt , T. Huse , R. S. Huston , D. Hutchcroft , D. Hynds , V. Iakovenko , P. Ilten , J. Imong , A. Inyakin , R. Jacobsson , A. Jaeger , M. Jahjah Hussein , E. Jans , F. Jansen , P. Jaton , B. Jean-Marie , F. Jing , M. John , D. Johnson , C. R. Jones , B. Jost , S. Kandybei , M. Karacson , T. M. Karbach , J. Keaveney , I. R. Kenyon , U. Kerzel , T. Ketel , A. Keune , B. Khanji , Y. M. Kim , M. Knecht , R. F. Koopman , P. Koppenburg , A. Kozlinskiy , L. Kravchuk , K. Kreplin , M. Kreps , G. Krocker , P. Krokovny , F. Kruse , K. Kruzelecki , M. Kucharczyk , T. Kvaratskheliya , V. N. La Thi , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , R. W. Lambert , E. Lanciotti , G. Lanfranchi , C. Langenbruch , T. Latham , C. Lazzeroni , R. Le Gac , J. van Leerdam , J. -P. Lees , A. Leflat , J. Lefrançois , R. Lefèvre , O. Leroy , T. Lesiak , L. Li , P. -R. Li , L. Li Gioi , M. Lieng , M. Liles , R. Lindner , C. Linn , B. Liu , G. Liu , J. von Loeben , J. H. Lopes , E. Lopez Asamar , N. Lopez-March , H. Lu , J. Luisier , X. Lyu , A. Mac Raighne , F. Machefert , F. Maciuc , O. Maev , S. Malde , R. M. D. Mamunur , G. Manca , G. Mancinelli , N. Mangiafave , J. F. Marchand , U. Marconi , J. Marks , G. Martellotti , A. Martens , L. Martin , D. Martinez Santos , A. Martín Sánchez , A. Massafferri , Z. Mathe , C. Matteuzzi , M. Matveev , E. Maurice , B. Maynard , A. Mazurov , G. McGregor , R. McNulty , M. Meissner , M. Merk , J. Merkel , R. Messi , S. Miglioranzi , D. A. Milanes , M. -N. Minard , J. Molina Rodriguez , S. Monteil , D. Moran , P. Morawski , R. Mountain , I. Mous , F. Muheim , R. Muresan , B. Muster , M. Musy , J. Mylroie-Smith , R. Märki , K. Müller , P. Naik , T. Nakada , R. Nandakumar , I. Nasteva , M. Nedos , M. Needham , N. Neufeld , A. D. Nguyen , C. Nguyen-Mau , M. Nicol , V. Niess , N. Nikitin , T. Nikodem , A. Nomerotski , A. Novoselov , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , S. Ogilvy , R. Oldeman , J. M. Otalora Goicochea , P. Owen , B. K. Pal , J. Palacios , A. Palano , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , C. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , S. K. Paterson , G. N. Patrick , C. Patrignani , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , D. L. Perego , P. Perret , M. Perrin-Terrin , A. Petrella , A. Petrolini , A. Phan , E. Picatoste Olloqui , B. Pie Valls , B. Pietrzyk , T. Pilař , D. Pinci , R. Plackett , S. Playfer , M. Plo Casasus , G. Polok , A. Poluektov , I. Polyakov , E. Polycarpo , D. Popov , B. Popovici , C. Potterat , A. Powell , J. Prisciandaro , V. Pugatch , A. Puig Navarro , A. Pérez-Calero Yzquierdo , W. Qian , J. H. Rademacker , B. Rakotomiaramanana , M. S. Rangel , I. Raniuk , G. Raven , S. Redford , M. M. Reid , A. C. dos Reis , S. Ricciardi , A. Richards , K. Rinnert , D. A. Roa Romero , P. Robbe , E. Rodrigues , P. Rodriguez Perez , G. J. Rogers , S. Roiser , V. Romanovskiy , J. Rouvinet , T. Ruf , H. Ruiz , G. Sabatino , J. J. Saborido Silva , N. Sagidova , P. Sail , B. Saitta , C. Salzmann , M. Sannino , R. Santacesaria , C. Santamarina Rios , R. Santinelli , E. Santovetti , M. Sapunov , A. Sarti , C. Satriano , A. Satta , M. Saur , D. Savrina , P. Schaack , M. Schiller , S. Schleich , M. Schlupp , M. Schmelling , B. Schmidt , O. Schneider , A. Schopper , M. H. Schune , R. Schwemmer , B. Sciascia , A. Sciubba , A. Semennikov , K. Senderowska , I. Sepp , N. Serra , J. Serrano , P. Seyfert , M. Shapkin , Y. Shcheglov , T. Shears , L. Shekhtman , V. Shevchenko , A. Shires , R. Silva Coutinho , T. Skwarnicki , E. Smith , K. Sobczak , F. J. P. Soler , A. Solomin , F. Soomro , B. Souza De Paula , B. Spaan , A. Sparkes , P. Spradlin , F. Stagni , S. Stahl , O. Steinkamp , O. Stenyakin , S. Stoica , S. Stone , B. Storaci , M. Straticiuc , U. Straumann , V. K. Subbiah , S. Swientek , M. Szczekowski , P. Szczypka , T. Szumlak , S. T'Jampens , E. Teodorescu , F. Teubert , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , N. Torr , E. Tournefier , S. Tourneur , M. T. Tran , A. Tsaregorodtsev , N. Tuning , M. Ubeda Garcia , A. Ukleja , P. Urquijo , U. Uwer , V. Vagnoni , G. Valenti , R. Vazquez Gomez , P. Vazquez Regueiro , S. Vecchi , J. J. Velthuis , M. Veltri , B. Viaud , I. Videau , D. Vieira , X. Vilasis-Cardona , J. Visniakov , A. Vollhardt , D. Volyanskyy , D. Voong , A. Vorobyev , S. Wandernoth , J. Wang , D. R. Ward , N. K. Watson , 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 , Z. Xing , Z. Yang , R. Young , O. Yushchenko , M. Zangoli , M. Zavertyaev , F. Zhang , L. Zhang , W. C. Zhang , Y. Zhang , A. Zhelezov , A. Zhokhov , L. Zhong , A. Zvyagin

In heavy ion collisions after the quark-gluon plasma there is a hadronic gas phase. Using effective Lagrangians we study the interactions of charmed mesons which lead to $J/\psi$ production and absorption in this gas. We update and extend…

High Energy Physics - Phenomenology · Physics 2018-04-11 L. M. Abreu , K. P. Khemchandani , A. Martínez Torres , F. S. Navarra , M. Nielsen

We consider a heavy quark-antiquark $(q\bar{q})$ pair as a heavy meson in the medium composed of light quarks and gluons. By using the AdS/CFT correspondence, the properties of this system are investigated. In particular, we study the…

High Energy Physics - Theory · Physics 2015-06-04 K. Bitaghsir Fadafan , E. Azimfard

We divide the cross section for a meson-meson reaction into three parts. The first part is for the quark-interchange process, the second for quark-antiquark annihilation processes and the third for resonant processes. Master rate equations…

Nuclear Theory · Physics 2011-06-08 Yu-Qi Li , Xiao-Ming Xu , Hui-Jun Ge

We study the dissociative associated production of a $J/\psi$ meson and a dimuon via double parton scattering (DPS) in nucleus--proton ultraperipheral collisions. This new channel, characterized by a rapidity gap, is sensitive to the photon…

High Energy Physics - Phenomenology · Physics 2026-05-11 Bruna O. Stahlhöfer , Edgar Huayra , Emmanuel G. de Oliveira

We analyze light meson electroproduction in the intermediate energy range where the quark contributions are essential. Our calculations are carried out on the basis of the handbag approach. We study cross sections and spin asymmetries for…

High Energy Physics - Phenomenology · Physics 2010-11-30 S. V. Goloskokov

We propose that the non-perturbative fragmentation functions describing the transition from a heavy quark to a heavy meson is proportional to the square of the produced meson wave function at the origin. We analyze the effects of this…

High Energy Physics - Phenomenology · Physics 2008-11-26 Fernando Cornet , Carlos A. Garcia Canal

The first observation of coherent $\phi$(1020) meson photoproduction off heavy nuclei is presented using ultraperipheral lead-lead collisions at a center-of-mass energy per nucleon pair of 5.36 TeV. The data were collected by the CMS…

Nuclear Experiment · Physics 2026-01-14 CMS Collaboration

We study the possibility to measure the elastic $\Phi N$ ($\Phi \equiv J/\psi, \psi(2S), \psi(3770),\chi_{2c}$) scattering cross section in the reaction $\bar p{+}d{\to}\Phi{+}n_{sp}$ and the elastic $D(\bar D) N$ scattering cross section…

Nuclear Theory · Physics 2015-06-26 W. Cassing , Ye. S. Golubeva , L. A. Kondratyuk

We calculate the differential cross section and single-polarization observables for the reaction $\gamma p \to \Phi p$ within perturbative QCD, treating the proton as a quark-diquark system. The phenomenological couplings of gauge bosons to…

High Energy Physics - Phenomenology · Physics 2009-10-31 C. F. Berger , W. Schweiger

We study the dissociation of $\psi (3770)$, $\psi (4040)$, $\psi (4160)$, and $\psi (4415)$ mesons in collisions with nucleons, which takes place in high-energy proton-nucleus collisions. Quark interchange between a nucleon and a $c\bar c$…

High Energy Physics - Phenomenology · Physics 2024-04-18 Ruo-Qing Ding , Xiao-Ming Xu , H. J. Weber

We study charm-strange mesons, or $D_s$, $D_s^*$, $D_{s0}^*(2317)$, and $D_{s1}(2460)$ mesons by focusing on their production by coalescence from a quark-gluon plasma in relativistic heavy ion collisions at $\sqrt{s_{NN}}=5.02$ TeV.…

Nuclear Theory · Physics 2025-10-22 Sungtae Cho , Su Houng Lee

We investigate the cold nuclear matter effects on $J/\psi$ production, whose understanding is fundamental to study the quark-gluon plasma. Two of these effects are of particular relevance: the shadowing of the parton distributions and the…

High Energy Physics - Phenomenology · Physics 2014-11-20 A. Rakotozafindrabe , E. G. Ferreiro , F. Fleuret , J. P. Lansberg

The ALICE Collaboration has studied the inclusive $\psi(\mathrm{2S})$ meson production in pp, p-Pb and Pb-Pb collisions at the CERN LHC. The $\psi(\mathrm{2S})$ is detected through its decay to a muon pair, using the forward Muon…

Nuclear Experiment · Physics 2019-08-13 Marco Leoncino

The production of J /{\psi} and {\Upsilon} mesons is studied in pp collisions at \surds = 7 TeV with the CMS experiment at the LHC. The J /{\psi} measurement is based on a dimuon sample corresponding to an integrated luminosity of 314…

High Energy Physics - Experiment · Physics 2011-09-07 Bora Akgün

The meson-photon transition form factors $\gamma\gamma^*\to P$ ($P$ stands for $\pi$, $\eta$ and $\eta'$) provide strong constraints on the distribution amplitudes of the pseudoscalar mesons. In this paper, these transition form factors are…

High Energy Physics - Phenomenology · Physics 2011-10-11 Xing-Gang Wu , Tao Huang