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We describe a new analysis of Upsilon(nS) to mu+mu- decays collected in proton anti-proton collisions with the CDF II detector at the Fermilab Tevatron. This analysis measures the angular distributions of the final state muons in the…

High Energy Physics - Experiment · Physics 2015-06-03 Matthew Jones

Differential production cross sections of J/$\psi$ and $\psi$(2S) charmonium and $\Upsilon$(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at $\sqrt{s} =$ 13 TeV, with data collected by the CMS detector at the…

High Energy Physics - Experiment · Physics 2018-03-16 CMS Collaboration

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 modification of the production of $J/\psi$, $\psi(\mathrm{2S})$, and $\mit{\Upsilon}(n\mathrm{S})$ ($n = 1, 2, 3$) in $p$+Pb collisions with respect to their production in $pp$ collisions has been studied. The $p$+Pb and $pp$ datasets…

Nuclear Experiment · Physics 2018-03-06 ATLAS Collaboration

The angular distributions of muons from Upsilon(1S,2S,3S) to mu+mu- decays are measured using data from proton anti-proton collisions at sqrt(s)=1.96 TeV corresponding to an integrated luminosity of 6.7 /fb and collected with the CDF II…

High Energy Physics - Experiment · Physics 2012-06-01 T. Aaltonen , B. Álvarez Gonzálezz , S. Amerio , D. Amidei , A. Anastassovx , A. Annovi , J. Antos , G. Apollinari , J. A. Appel , T. Arisawa , A. Artikov , J. Asaadi , W. Ashmanskas , B. Auerbach , A. Aurisano , F. Azfar , W. Badgett , T. Bae , A. Barbaro-Galtieri , V. E. Barnes , B. A. Barnett , P. Barriahh , P. Bartos , M. Bauceff , F. Bedeschi , S. Behari , G. Bellettinigg , J. Bellinger , D. Benjamin , A. Beretvas , A. Bhatti , D. Biselloff , I. Bizjak , K. R. Bland , B. Blumenfeld , A. Bocci , A. Bodek , D. Bortoletto , J. Boudreau , A. Boveia , L. Brigliadoriee , C. Bromberg , E. Brucken , J. Budagov , H. S. Budd , K. Burkett , G. Busettoff , P. Bussey , A. Buzatu , A. Calamba , C. Calancha , S. Camarda , M. Campanelli , M. Campbell , F. Canelli , B. Carls , D. Carlsmith , R. Carosi , S. Carrillom , S. Carron , B. Casalk , M. Casarsa , A. Castroee , P. Catastini , D. Cauz , V. Cavaliere , M. Cavalli-Sforza , A. Cerrif , L. Cerritos , Y. C. Chen , M. Chertok , G. Chiarelli , G. Chlachidze , F. Chlebana , K. Cho , D. Chokheli , W. H. Chung , Y. S. Chung , M. A. Cioccihh , A. Clark , C. Clarke , G. Compostellaff , M. E. Convery , J. Conway , M. Corbo , M. Cordelli , C. A. Cox , D. J. Cox , F. Crescioligg , J. Cuevasz , R. Culbertson , D. Dagenhart , N. d'Ascenzow , M. Datta , P. de Barbaro , M. Dell'Orsogg , L. Demortier , M. Deninno , F. Devoto , M. d'Erricoff , A. Di Cantogg , B. Di Ruzza , J. R. Dittmann , M. D'Onofrio , S. Donatigg , P. Dong , M. Dorigo , T. Dorigo , K. Ebina , A. Elagin , A. Eppig , R. Erbacher , S. Errede , N. Ershaidatdd , R. Eusebi , S. Farrington , M. Feindt , J. P. Fernandez , R. Field , G. Flanaganu , R. Forrest , M. J. Frank , M. Franklin , J. C. Freeman , Y. Funakoshi , I. Furic , M. Gallinaro , J. E. Garcia , A. F. Garfinkel , P. Garosihh , H. Gerberich , E. Gerchtein , S. Giagu , V. Giakoumopoulou , P. Giannetti , K. Gibson , C. M. Ginsburg , N. Giokaris , P. Giromini , G. Giurgiu , V. Glagolev , D. Glenzinski , M. Gold , D. Goldin , N. Goldschmidt , A. Golossanov , G. Gomez , G. Gomez-Ceballos , M. Goncharov , O. González , I. Gorelov , A. T. Goshaw , K. Goulianos , S. Grinstein , C. Grosso-Pilcher , R. C. Group , J. Guimaraes da Costa , S. R. Hahn , E. Halkiadakis , A. Hamaguchi , J. Y. Han , F. Happacher , K. Hara , D. Hare , M. Hare , R. F. Harr , K. Hatakeyama , C. Hays , M. Heck , J. Heinrich , M. Herndon , S. Hewamanage , A. Hocker , W. Hopkinsg , D. Horn , S. Hou , R. E. Hughes , M. Hurwitz , U. Husemann , N. Hussain , M. Hussein , J. Huston , G. Introzzi , M. Iorijj , A. Ivanovp , E. James , D. Jang , B. Jayatilaka , E. J. Jeon , S. Jindariani , M. Jones , K. K. Joo , S. Y. Jun , T. R. Junk , T. Kamon , P. E. Karchin , A. Kasmi , Y. Katoo , W. Ketchum , J. Keung , V. Khotilovich , B. Kilminster , D. H. Kim , H. S. Kim , J. E. Kim , M. J. Kim , S. B. Kim , S. H. Kim , Y. K. Kim , Y. J. Kim , N. Kimura , M. Kirby , S. Klimenko , K. Knoepfel , K. Kondo , D. J. Kong , J. Konigsberg , A. V. Kotwal , M. Kreps , J. Kroll , D. Krop , M. Kruse , V. Krutelyovc , T. Kuhr , M. Kurata , S. Kwang , A. T. Laasanen , S. Lami , S. Lammel , M. Lancaster , R. L. Lander , K. Lannony , A. Lath , G. Latinohh , T. LeCompte , E. Lee , H. S. Leeq , J. S. Lee , S. W. Leebb , S. Leogg , S. Leone , J. D. Lewis , A. Limosanit , C. -J. Lin , M. Lindgren , E. Lipeles , A. Lister , D. O. Litvintsev , C. Liu , H. Liu , Q. Liu , T. Liu , S. Lockwitz , A. Loginov , D. Lucchesiff , J. Lueck , P. Lujan , P. Lukens , G. Lungu , J. Lys , R. Lysake , R. Madrak , K. Maeshima , P. Maestrohh , S. Malik , G. Mancaa , A. Manousakis-Katsikakis , F. Margaroli , C. Marino , M. Martínez , P. Mastrandrea , K. Matera , M. E. Mattson , A. Mazzacane , P. Mazzanti , K. S. McFarland , P. McIntyre , R. McNultyj , A. Mehta , P. Mehtala , C. Mesropian , T. Miao , D. Mietlicki , A. Mitra , H. Miyake , S. Moed , N. Moggi , M. N. Mondragonm , C. S. Moon , R. Moore , M. J. Morelloii , J. Morlock , P. Movilla Fernandez , A. Mukherjee , Th. Muller , P. Murat , M. Mussiniee , J. Nachtmann , Y. Nagai , J. Naganoma , I. Nakano , A. Napier , J. Nett , C. Neu , M. S. Neubauer , J. Nielsend , L. Nodulman , S. Y. Noh , O. Norniella , L. Oakes , S. H. Oh , Y. D. Oh , I. Oksuzian , T. Okusawa , R. Orava , L. Ortolan , S. Pagan Grisoff , C. Pagliarone , E. Palenciaf , V. Papadimitriou , A. A. Paramonov , J. Patrick , G. Paulettakk , M. Paulini , C. Paus , D. E. Pellett , A. Penzo , T. J. Phillips , G. Piacentino , E. Pianori , J. Pilot , K. Pitts , C. Plager , L. Pondrom , S. Poprockig , K. Potamianos , F. Prokoshincc , A. Pranko , F. Ptohosh , G. Punzigg , A. Rahaman , V. Ramakrishnan , N. Ranjan , I. Redondo , P. Renton , M. Rescigno , T. Riddick , F. Rimondiee , L. Ristori , A. Robson , T. Rodrigo , T. Rodriguez , E. Rogers , S. Rollii , R. Roser , F. Ruffinihh , A. Ruiz , J. Russ , V. Rusu , A. Safonov , W. K. Sakumoto , Y. Sakurai , L. Santikk , K. Sato , V. Savelievw , A. Savoy-Navarroaa , P. Schlabach , A. Schmidt , E. E. Schmidt , T. Schwarz , L. Scodellaro , A. Scribanohh , F. Scuri , S. Seidel , Y. Seiya , A. Semenov , F. Sforzahh , S. Z. Shalhout , T. Shears , P. F. Shepard , M. Shimojimav , M. Shochet , I. Shreyber-Tecker , A. Simonenko , P. Sinervo , K. Sliwa , J. R. Smith , F. D. Snider , A. Soha , V. Sorin , H. Song , P. Squillaciotihh , M. Stancari , R. St. Denis , B. Stelzer , O. Stelzer-Chilton , D. Stentzx , J. Strologas , G. L. Strycker , Y. Sudo , A. Sukhanov , I. Suslov , K. Takemasa , Y. Takeuchi , J. Tang , M. Tecchio , P. K. Teng , J. Thomg , J. Thome , G. A. Thompson , E. Thomson , D. Toback , S. Tokar , K. Tollefson , T. Tomura , D. Tonelli , S. Torre , D. Torretta , P. Totaro , M. Trovatoii , F. Ukegawa , S. Uozumi , A. Varganov , F. Vázquezm , G. Velev , C. Vellidis , M. Vidal , I. Vila , R. Vilar , J. Vizán , M. Vogel , G. Volpi , P. Wagner , R. L. Wagner , T. Wakisaka , R. Wallny , S. M. Wang , A. Warburton , D. Waters , W. C. Wester , D. Whitesonb , A. B. Wicklund , E. Wicklund , S. Wilbur , F. Wick , H. H. Williams , J. S. Wilson , P. Wilson , B. L. Winer , P. Wittichg , S. Wolbers , H. Wolfe , T. Wright , X. Wu , Z. Wu , K. Yamamoto , D. Yamato , T. Yang , U. K. Yangr , Y. C. Yang , W. -M. Yao , G. P. Yeh , K. Yin , J. Yoh , K. Yorita , T. Yoshidal , G. B. Yu , I. Yu , S. S. Yu , J. C. Yun , A. Zanetti , Y. Zeng , C. Zhou , S. Zucchelliee

We investigate the inclusive production of double quarkonia ($J/\psi$, $\psi(2S)$, $\Upsilon$ mesons) in polarized hadron-hadron collisions, considering the kinematic configuration where the transverse momentum of each pair of bound states…

High Energy Physics - Phenomenology · Physics 2026-02-09 Carlo Flore , Cristian Pisano

The production of quarkonium is an important testing ground for QCD calculations. The J/\psi\ and \Upsilon\ production cross-sections are measured in proton-proton collisions at a centre-of-mass energy of 7~TeV with the ATLAS detector at…

High Energy Physics - Experiment · Physics 2015-06-03 Darren D Price

This article reports on the inclusive production cross section of several quarkonium states, $\mathrm{J}/\psi$, $\psi {\rm (2S)}$, $\Upsilon\rm(1S)$, $\Upsilon\rm(2S)$, and $\Upsilon\rm(3S)$, measured with the ALICE detector at the LHC, in…

Nuclear Experiment · Physics 2023-03-01 ALICE Collaboration

We present a measurement of the polarization observed for bottomonium states produced in p-Cu collisions at sqrt(s)=38.8 GeV. The angular distribution of the decay dimuons of the Upsilon(1S) state show no polarization at small xF and pT but…

The polarizations of Y(nS) (n=1,2,3) and prompt J/\psi and \psi(2S), as well as the differential cross section of the Y(nS), are measured in proton-proton collisions at sqrt(s) = 7 TeV, using a dimuon data sample collected by the CMS…

High Energy Physics - Experiment · Physics 2013-12-02 Linlin Zhang

Several fixed-target experiments reported J/$\psi$ and $\Upsilon$ polarization measurements, as functions of Feynman $x$ ($x_{\rm F}$) and transverse momentum ($p_{\rm T}$), in three different polarization frames, using different…

High Energy Physics - Phenomenology · Physics 2022-10-19 Pietro Faccioli , Ilse Krätschmer , Carlos Lourenço

Both charm and bottom quarks form nonrelativistic bound states analogous to positronium. The J/psi and psi(2S) charmonium states and the first three Upsilon(nS) bottomonium states, all spin-triplet S-wave quarkonium states below…

High Energy Physics - Experiment · Physics 2015-06-18 Eric Braaten , James Russ

The inclusive production cross sections at forward rapidity of J/$\psi$, $\psi$(2S), $\Upsilon$(1S) and $\Upsilon$(2S) are measured in pp collisions at $\sqrt{s} = 7$ TeV with the ALICE detector at the LHC. The analysis is based in a data…

Nuclear Experiment · Physics 2014-09-10 ALICE Collaboration

About 40-50 % of the quarkonium ground states J/psi(1S) and Upsilon(1S) produced in hadronic collisions originate from the decay of higher excitations. In a hot medium, these higher states are dissociated at lower temperatures than the more…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. Digal , P. Petreczky , H. Satz

This talk presents a review of recent results for quarkonium production at the LHC from ATLAS, CMS, LHCb, and ALICE. Production cross sections for $J/\psi$, $\psi(2S)$, and $\Upsilon(mS)$, and production ratios for $\chi_{c,bJ}$ are found…

High Energy Physics - Experiment · Physics 2014-09-10 Bryan Fulsom

We report on the inclusive production cross sections of J/$\psi$, $\psi$(2S), $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S), measured at forward rapidity with the ALICE detector in pp collisions at a center-of-mass energy $\sqrt{s}=8$…

High Energy Physics - Experiment · Physics 2016-05-27 ALICE Collaboration

Two recent analyses of data collected with the ATLAS detector at the Large Hadron Collider are presented. In the first, a measurement of $b$ hadron pair production is presented, based on a data set corresponding to an integrated luminosity…

High Energy Physics - Experiment · Physics 2019-05-31 Sally Seidel

The chi_b(nP) quarkonium states are produced in proton-proton collisions at the Large Hadron Collider (LHC) at sqrt(s) = 7 TeV and recorded by the ATLAS detector. Using a data sample corresponding to an integrated luminosity of 4.4 fb^-1,…

High Energy Physics - Experiment · Physics 2013-06-25 ATLAS Collaboration

The angular distributions of Upsilon(1S) to mu+ mu- decays are analyzed using a sample of Upsilon(1S) mesons in 2.9 fb^{-1} of data collected at sqrt{s} = 1.96TeV. The results of the one-dimensional angular analysis suggest that Upsilon(1S)…

High Energy Physics - Experiment · Physics 2011-10-04 Niharika Ranjan

The ATLAS detector at CERN's LHC is preparing to take data from the first proton-proton collisions expected in the next few months. We report on the analysis of simulated data samples for production of heavy Quarkonium states J/psi and…

High Energy Physics - Experiment · Physics 2014-11-18 Erez Etzion , Jony Ginzburg
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