English
Related papers

Related papers: Inclusive Charm Production in Upsilon(nS) Decay

200 papers

In relativistic nuclear collisions the production of hadrons with light (u,d,s) quarks is quantitatively described in the framework of the Statistical Hadronization Model (SHM). Charm quarks are dominantly produced in initial hard…

We calculate the decay rate of bottomonium to two-charm quark jets $\Upsilon \to c \bar c$ at the tree level and one-loop level including color-singlet and color-octet $b \bar b$ annihilations. We find that the short distance coefficient of…

High Energy Physics - Phenomenology · Physics 2009-02-23 Yu-Jie Zhang , Kuang-Ta Chao

We give results for the Upsilon spectrum from lattice QCD using an improved version of the NRQCD action for b quarks which includes radiative corrections to kinetic terms at O(v^4) in the velocity expansion. We also include for the first…

We present $O(\alpha_s^2)$ QCD corrections to the fully-differential decay rate of a $b$-quark into inclusive semileptonic charmless final states. Our calculation provides genuine two-loop QCD corrections, beyond the…

High Energy Physics - Phenomenology · Physics 2015-06-12 Mathias Brucherseifer , Fabrizio Caola , Kirill Melnikov

We use a recently proposed non-perturbative model, based on an effective strong coupling constant and free from tunable parameters, to study c-flavoured hadron production in e+e- annihilation. Charm-quark production is described in the…

High Energy Physics - Phenomenology · Physics 2010-03-25 Gennaro Corcella , Giancarlo Ferrera

Background: Intrinsic charm, nonperturbative charm in the hadron wavefunction, has long been speculated but has never been satisfactorily proven. Open charm and $J/\psi$ measurements in a fixed-taget configuration at the LHCb searched for…

High Energy Physics - Phenomenology · Physics 2023-09-06 R. Vogt

First observations of the decays $\Lambda_b^0 \to \Lambda_c^+ D_{(s)}^-$ are reported using data corresponding to an integrated luminosity of $3\,{\rm fb}^{-1}$ collected at 7 and 8 TeV center-of-mass energy in proton-proton collisions with…

High Energy Physics - Experiment · Physics 2016-03-27 LHCb collaboration , R. Aaij , A. Abba , B. Adeva , M. Adinolfi , A. Affolder , Z. Ajaltouni , J. Albrecht , F. Alessio , M. Alexander , S. Ali , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , S. Amerio , Y. Amhis , L. An , L. Anderlini , J. Anderson , R. Andreassen , M. Andreotti , J. E. Andrews , R. B. Appleby , O. Aquines Gutierrez , F. Archilli , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , M. Baalouch , S. Bachmann , J. J. Back , A. Badalov , V. Balagura , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , V. Batozskaya , Th. Bauer , A. Bay , J. Beddow , F. Bedeschi , I. Bediaga , S. Belogurov , K. Belous , I. Belyaev , E. Ben-Haim , G. Bencivenni , S. Benson , J. Benton , A. Berezhnoy , R. Bernet , M. -O. Bettler , M. van Beuzekom , A. Bien , S. Bifani , T. Bird , A. Bizzeti , P. M. Bjørnstad , T. Blake , F. Blanc , J. Blouw , S. Blusk , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , A. Borgia , M. Borsato , T. J. V. Bowcock , E. Bowen , C. Bozzi , T. Brambach , J. van den Brand , J. Bressieux , D. Brett , M. Britsch , T. Britton , N. H. Brook , H. Brown , A. Bursche , G. Busetto , J. Buytaert , S. Cadeddu , R. Calabrese , O. Callot , M. Calvi , M. Calvo Gomez , A. Camboni , P. Campana , D. Campora Perez , F. Caponio , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , H. Carranza-Mejia , L. Carson , K. Carvalho Akiba , G. Casse , L. Cassina , L. Castillo Garcia , M. Cattaneo , Ch. Cauet , R. Cenci , M. Charles , Ph. Charpentier , S. -F. Cheung , N. Chiapolini , M. Chrzaszcz , K. Ciba , X. Cid Vidal , G. Ciezarek , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , C. Coca , V. Coco , J. Cogan , E. Cogneras , P. Collins , A. Comerma-Montells , A. Contu , A. Cook , M. Coombes , S. Coquereau , G. Corti , M. Corvo , I. Counts , B. Couturier , G. A. Cowan , D. C. Craik , M. Cruz Torres , A. R. Cukierman , S. Cunliffe , R. Currie , C. D'Ambrosio , J. Dalseno , P. David , P. N. Y. David , A. Davis , K. De Bruyn , S. De Capua , M. De Cian , J. M. De Miranda , L. De Paula , W. De Silva , P. De Simone , D. Decamp , M. Deckenhoff , L. Del Buono , N. Déléage , D. Derkach , O. Deschamps , F. Dettori , A. Di Canto , H. Dijkstra , S. Donleavy , F. Dordei , M. Dorigo , C. Dorothy , A. Dosil Suárez , D. Dossett , A. Dovbnya , F. Dupertuis , P. Durante , R. Dzhelyadin , A. Dziurda , A. Dzyuba , S. Easo , U. Egede , V. Egorychev , S. Eidelman , S. Eisenhardt , U. Eitschberger , R. Ekelhof , L. Eklund , I. El Rifai , Ch. Elsasser , S. Esen , T. Evans , A. Falabella , C. Färber , C. Farinelli , S. Farry , D. Ferguson , V. Fernandez Albor , F. Ferreira Rodrigues , M. Ferro-Luzzi , S. Filippov , M. Fiore , M. Fiorini , M. Firlej , C. Fitzpatrick , T. Fiutowski , M. Fontana , F. Fontanelli , R. Forty , O. Francisco , M. Frank , C. Frei , M. Frosini , J. Fu , E. Furfaro , A. Gallas Torreira , D. Galli , S. Gambetta , M. Gandelman , P. Gandini , Y. Gao , J. Garofoli , J. Garra Tico , L. Garrido , C. Gaspar , R. Gauld , L. Gavardi , E. Gersabeck , M. Gersabeck , T. Gershon , Ph. Ghez , A. Gianelle , S. Giani' , V. Gibson , L. Giubega , V. V. Gligorov , C. Göbel , 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 , P. Griffith , L. Grillo , O. Grünberg , B. Gui , E. Gushchin , Yu. Guz , T. Gys , C. Hadjivasiliou , G. Haefeli , C. Haen , S. C. Haines , S. Hall , B. Hamilton , T. Hampson , X. Han , S. Hansmann-Menzemer , N. Harnew , S. T. Harnew , J. Harrison , T. Hartmann , J. He , T. Head , V. Heijne , K. Hennessy , P. Henrard , L. Henry , J. A. Hernando Morata , E. van Herwijnen , M. Heß , A. Hicheur , D. Hill , M. Hoballah , C. Hombach , W. Hulsbergen , P. Hunt , N. Hussain , D. Hutchcroft , D. Hynds , M. Idzik , P. Ilten , R. Jacobsson , A. Jaeger , J. Jalocha , E. Jans , P. Jaton , A. Jawahery , M. Jezabek , F. Jing , M. John , D. Johnson , C. R. Jones , C. Joram , B. Jost , N. Jurik , M. Kaballo , S. Kandybei , W. Kanso , M. Karacson , T. M. Karbach , M. Kelsey , I. R. Kenyon , T. Ketel , B. Khanji , C. Khurewathanakul , S. Klaver , O. Kochebina , M. Kolpin , I. Komarov , R. F. Koopman , P. Koppenburg , M. Korolev , A. Kozlinskiy , L. Kravchuk , K. Kreplin , M. Kreps , G. Krocker , P. Krokovny , F. Kruse , M. Kucharczyk , V. Kudryavtsev , K. Kurek , T. Kvaratskheliya , V. N. La Thi , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , R. W. Lambert , E. Lanciotti , G. Lanfranchi , C. Langenbruch , B. Langhans , T. Latham , C. Lazzeroni , R. Le Gac , J. van Leerdam , J. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , S. Leo , O. Leroy , T. Lesiak , B. Leverington , Y. Li , M. Liles , R. Lindner , C. Linn , F. Lionetto , B. Liu , G. Liu , S. Lohn , I. Longstaff , I. Longstaff , J. H. Lopes , N. Lopez-March , P. Lowdon , H. Lu , D. Lucchesi , H. Luo , A. Lupato , E. Luppi , O. Lupton , F. Machefert , I. V. Machikhiliyan , F. Maciuc , O. Maev , S. Malde , G. Manca , G. Mancinelli , M. Manzali , J. Maratas , J. F. Marchand , U. Marconi , C. Marin Benito , P. Marino , R. Märki , J. Marks , G. Martellotti , A. Martens , A. Martín Sánchez , M. Martinelli , D. Martinez Santos , F. Martinez Vidal , D. Martins Tostes , A. Massafferri , R. Matev , Z. Mathe , C. Matteuzzi , A. Mazurov , M. McCann , J. McCarthy , A. McNab , R. McNulty , B. McSkelly , B. Meadows , F. Meier , M. Meissner , M. Merk , D. A. Milanes , M. -N. Minard , J. Molina Rodriguez , S. Monteil , D. Moran , M. Morandin , P. Morawski , A. Mordà , M. J. Morello , J. Moron , R. Mountain , F. Muheim , K. Müller , R. Muresan , B. Muster , P. Naik , T. Nakada , R. Nandakumar , I. Nasteva , M. Needham , N. Neri , S. Neubert , N. Neufeld , M. Neuner , A. D. Nguyen , T. D. Nguyen , C. Nguyen-Mau , M. Nicol , V. Niess , R. Niet , N. Nikitin , T. Nikodem , A. Novoselov , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , S. Ogilvy , O. Okhrimenko , R. Oldeman , G. Onderwater , M. Orlandea , J. M. Otalora Goicochea , P. Owen , A. Oyanguren , B. K. Pal , A. Palano , F. Palombo , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , C. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , C. Patrignani , A. Pazos Alvarez , A. Pearce , A. Pellegrino , M. Pepe Altarelli , S. Perazzini , E. Perez Trigo , P. Perret , M. Perrin-Terrin , L. Pescatore , E. Pesen , K. Petridis , A. Petrolini , E. Picatoste Olloqui , B. Pietrzyk , T. Pilař , D. Pinci , A. Pistone , S. Playfer , M. Plo Casasus , F. Polci , A. Poluektov , E. Polycarpo , A. Popov , D. Popov , B. Popovici , C. Potterat , A. Powell , J. Prisciandaro , A. Pritchard , C. Prouve , V. Pugatch , A. Puig Navarro , G. Punzi , W. Qian , B. Rachwal , J. H. Rademacker , B. Rakotomiaramanana , M. Rama , M. S. Rangel , I. Raniuk , N. Rauschmayr , G. Raven , S. Reichert , M. M. Reid , A. C. dos Reis , S. Ricciardi , A. Richards , K. Rinnert , V. Rives Molina , D. A. Roa Romero , P. Robbe , A. B. Rodrigues , E. Rodrigues , P. Rodriguez Perez , S. Roiser , V. Romanovsky , A. Romero Vidal , M. Rotondo , J. Rouvinet , T. Ruf , F. Ruffini , H. Ruiz , P. Ruiz Valls , G. Sabatino , J. J. Saborido Silva , N. Sagidova , P. Sail , B. Saitta , V. Salustino Guimaraes , C. Sanchez Mayordomo , B. Sanmartin Sedes , R. Santacesaria , C. Santamarina Rios , E. Santovetti , M. Sapunov , A. Sarti , C. Satriano , A. Satta , M. Savrie , D. Savrina , M. Schiller , H. Schindler , M. Schlupp , M. Schmelling , B. Schmidt , O. Schneider , A. Schopper , M. -H. Schune , R. Schwemmer , B. Sciascia , A. Sciubba , M. Seco , A. Semennikov , K. Senderowska , I. Sepp , N. Serra , J. Serrano , L. Sestini , P. Seyfert , M. Shapkin , I. Shapoval , Y. Shcheglov , T. Shears , L. Shekhtman , V. Shevchenko , A. Shires , R. Silva Coutinho , G. Simi , M. Sirendi , N. Skidmore , T. Skwarnicki , N. A. Smith , E. Smith , E. Smith , J. Smith , M. Smith , H. Snoek , M. D. Sokoloff , F. J. P. Soler , F. Soomro , D. Souza , B. Souza De Paula , B. Spaan , A. Sparkes , F. Spinella , P. Spradlin , F. Stagni , S. Stahl , O. Steinkamp , O. Stenyakin , S. Stevenson , S. Stoica , S. Stone , B. Storaci , S. Stracka , M. Straticiuc , U. Straumann , R. Stroili , V. K. Subbiah , L. Sun , W. Sutcliffe , K. Swientek , S. Swientek , V. Syropoulos , M. Szczekowski , P. Szczypka , D. Szilard , T. Szumlak , S. T'Jampens , M. Teklishyn , G. Tellarini , E. Teodorescu , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , S. Tolk , L. Tomassetti , D. Tonelli , S. Topp-Joergensen , N. Torr , E. Tournefier , S. Tourneur , M. T. Tran , M. Tresch , A. Tsaregorodtsev , P. Tsopelas , N. Tuning , M. Ubeda Garcia , A. Ukleja , A. Ustyuzhanin , U. Uwer , V. Vagnoni , G. Valenti , A. Vallier , R. Vazquez Gomez , P. Vazquez Regueiro , C. Vázquez Sierra , S. Vecchi , J. J. Velthuis , M. Veltri , G. Veneziano , M. Vesterinen , B. Viaud , D. Vieira , M. Vieites Diaz , X. Vilasis-Cardona , A. Vollhardt , D. Volyanskyy , D. Voong , A. Vorobyev , V. Vorobyev , C. Voß , H. Voss , J. A. de Vries , R. Waldi , C. Wallace , R. Wallace , J. Walsh , S. Wandernoth , J. Wang , D. R. Ward , N. K. Watson , A. D. Webber , D. Websdale , M. Whitehead , J. Wicht , D. Wiedner , G. Wilkinson , M. P. Williams , M. Williams , F. F. Wilson , J. Wimberley , J. Wishahi , W. Wislicki , M. Witek , G. Wormser , S. A. Wotton , S. Wright , S. Wu , K. Wyllie , Y. Xie , Z. Xing , Z. Xu , Z. Yang , X. Yuan , O. Yushchenko , M. Zangoli , M. Zavertyaev , F. Zhang , L. Zhang , W. C. Zhang , Y. Zhang , A. Zhelezov , A. Zhokhov , L. Zhong , A. Zvyagin

In this paper, we study the $J/\psi(\Upsilon)$ production in Z boson decay in color-singlet model(CSM). We calculate the next-to-leading-order (NLO) QCD correction to $Z \to Quarkonium+Q\bar{Q}$, the dominant contribution in the CSM, with…

High Energy Physics - Phenomenology · Physics 2014-11-21 Rong Li , Jian-Xiong Wang

We present our new measurement of the cross-section for charm dimuon production in neutrino-iron interactions based upon the full statistics collected by the NOMAD experiment. After background subtraction we observe 15,344 charm dimuon…

High Energy Physics - Experiment · Physics 2013-08-23 NOMAD Collaboration

We propose a method to non-perturbatively calculate the forward-scattering matrix elements relevant to inclusive semi-leptonic B meson decays. Corresponding hadronic structure functions at unphysical kinematics are accessible through…

High Energy Physics - Lattice · Physics 2019-12-06 Shoji Hashimoto

Charm and bottom production near threshold is sensitive to the multi-quark, gluonic, and hidden-color correlations of hadronic and nuclear wavefunctions in QCD since all of the target's constituents must act coherently within the small…

High Energy Physics - Phenomenology · Physics 2009-09-11 S. J. Brodsky , E. Chudakov , P. Hoyer , J. M. Laget

The role of the charm quark in the dynamics underlying the \Delta I = 1/2 rule for kaon decays can be understood by studying the dependence of kaon decay amplitudes on the charm quark mass using an effective \Delta S = 1 weak Hamiltonian in…

High Energy Physics - Lattice · Physics 2012-10-23 Eric Endress , Carlos Pena

The charm quark has unique properties that make it a very important probe of many facets of the Standard Model. New experimental information on charm decays is becoming available from dedicated experiments at charm factories, and through…

High Energy Physics - Experiment · Physics 2010-11-05 M. Artuso

In the paper, we derive the next-to-leading order (NLO) fragmentation function for a heavy quark, either charm or bottom, into a heavy quarkonium $J/\Psi$ or $\Upsilon$. The ultra-violet divergences in the real corrections are removed…

High Energy Physics - Phenomenology · Physics 2019-07-17 Xu-Chang Zheng , Chao-Hsi Chang , Xing-Gang Wu

We calculate open charm production in $Pb+Pb$ reactions at SPS energies within the HSD transport approach - which is based on string, quark, diquark ($q, \bar{q}, qq, \bar{q}\bar{q}$) and hadronic degrees of freedom - including the…

High Energy Physics - Phenomenology · Physics 2009-11-07 W. Cassing , L. A. Kondratyuk , G. I. Lykasov , M. V. Rzjanin

We introduce a new method for the determination of the ratio of production fractions $R^{\pm0}=\mathcal B(\Upsilon(4S)\to B^+B^-)/\mathcal B(\Upsilon(4S)\to B^0\bar B^0)$ based on $\bar B\to D^{(*)}\ell\bar \nu$ decays. Given the importance…

High Energy Physics - Phenomenology · Physics 2026-04-10 Martin Jung , Stefan Schacht

Within the framework of nonrelativistic QCD (NRQCD), we calculate the fragmentation function for a charm quark into an $S$-wave fully-charmed tetraquark, denoted as $T_{4c}$. The charm-to-$T_{4c}$ fragmentation function is expressed as a…

High Energy Physics - Phenomenology · Physics 2024-09-04 Xiao-Wei Bai , Feng Feng , Chang-Man Gan , Yingsheng Huang , Wen-Long Sang , Hong-Fei Zhang

Recent measurements of J/psi production in e^+ e^- colliders pose a challenge to the NRQCD factorization theorem for quarkonium production. Discrepancies between leading order calculations of color-octet contributions and the momentum…

High Energy Physics - Phenomenology · Physics 2014-11-17 Thomas Mehen

A summary of charm hadron production fractions is given, as measured at e+e- storage rings and at HERA, taking into account the newest values of charmed hadron decay branching ratios.

High Energy Physics - Experiment · Physics 2011-12-19 E. Lohrmann

Inspired by the potential prospects of ${\Upsilon}(nS)$ data samples ($n$ $=$ $1$, $2$, $3$) at LHC and SuperKEKB, ${\Upsilon}(nS)$ ${\to}$ $B_{c}{\rho}$, $B_{c}K^{\ast}$ decays are studied phenomenologically with pQCD approach. Branching…

High Energy Physics - Phenomenology · Physics 2017-10-02 Junfeng Sun , Yueling Yang , Jinshu Huang , Gongru Lu , Qin Chang
‹ Prev 1 8 9 10 Next ›