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By combining potential models and QCD spectral sum rules (QSSR), we discuss the spectroscopy of the $(b\bar c)$ mesons and of the $(bcq)$, $(ccq)$ and $(bbq)$ baryons (${q}\equiv {d}$ or $s$), the decay constant and the (semi)leptonic decay…

High Energy Physics - Phenomenology · Physics 2014-09-17 E. Bagan , H. G. Dosch , P. Gosdzinsky , S. Narison , J. M. Richard

The hadronic weak decays of $\Lambda_c$ are studied in the framework of a constituent quark model. With the combined analysis of the Cabbibo-favored processes, $\Lambda_c\to \Lambda\pi^+$, $\Sigma^0\pi^+$ and $\Sigma^+\pi^0$, we confirm…

High Energy Physics - Phenomenology · Physics 2020-10-21 Peng-Yu Niu , Jean-Marc Richard , Qian Wang , Qiang Zhao

In general-mass variable-flavor-number (GM-VFN) scheme, the `heavy quark mechanisms' of $B_c(B_c^*)$ meson hadroproduction via the sub-processes $g+c\to B_c(B_c^*)+...$ and $g+\bar{b}\to B_c(B_c^*)+...$ are investigated. In the scheme,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chao-Hsi Chang , Cong-Feng Qiao , Jian-Xiong Wang , Xing-Gang Wu

In the framework of potential models for heavy quarkonium the mass spectrum for the system ($\bar b c$) is considered. Spin-dependent splittings, taking into account a change of a constant for effective Coulomb interaction between the…

High Energy Physics - Phenomenology · Physics 2009-10-28 V. V. Kiselev , A. K. Likhoded , A. V. Tkabladze

To the leading order, the radiative leptonic decays $B_c \to \gamma \ell \bar \nu$ ($ \ell=e, \mu$) are studied carefully. In the study, a non-relativistic constituent quark model and the effective Lagrangian for the heavy flavour decays…

High Energy Physics - Phenomenology · Physics 2009-10-30 Chao-Hsi Chang , Jian-Ping Cheng , Cai-Dian Lu

Decays of b hadrons into final states containing a D0 meson and a muon are used to measure the b anti-b production cross-section in proton-proton collisions at a centre-of-mass energy of 7 TeV at the LHC. In the pseudorapidity interval 2 <…

High Energy Physics - Experiment · Physics 2012-07-20 LHCb Collaboration , R. Aaij , C. Abellan Beteta , B. Adeva , M. Adinolfi , C. Adrover , A. Affolder , M. Agari , Z. Ajaltouni , J. Albrecht , F. Alessio , M. Alexander , M. Alfonsi , P. Alvarez Cartelle , A. A. Alves , S. Amato , Y. Amhis , J. Amoraal , J. Anderson , R. Antunes Nobrega , R. Appleby , O. Aquines Gutierrez , A. Arefyev , L. Arrabito , M. Artuso , E. Aslanides , G. Auriemma , S. Bachmann , Y. Bagaturia , D. S. Bailey , V. Balagura , W. Baldini , G. Barber , C. Barham , R. J. Barlow , S. Barsuk , S. Basiladze , A. Bates , C. Bauer , Th. Bauer , A. Bay , I. Bediaga , T. Bellunato , K. Belous , I. Belyaev , M. Benayoun , G. Bencivenni , R. Bernet , R. P. Bernhard , M. -O. Bettler , M. van Beuzekom , J. H. Bibby , S. Bifani , A. Bizzeti , P. M. Bjørnstad , T. Blake , F. Blanc , C. Blanks , J. Blouw , S. Blusk , A. Bobrov , V. Bocci , B. Bochin , E. Bonaccorsi , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , A. Borgia , E. Bos , T. J. V. Bowcock , C. Bozzi , T. Brambach , J. van den Brand , L. Brarda , J. Bressieux , S. Brisbane , M. Britsch , N. H. Brook , H. Brown , S. Brusa , A. Büchler-Germann , A. Bursche , J. Buytaert , S. Cadeddu , J. M. Caicedo Carvajal , O. Callot , M. Calvi , M. Calvo Gomez , A. Camboni , W. Cameron , L. Camilleri , P. Campana , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , J. Carroll , L. Carson , K. Carvalho Akiba , G. Casse , M. Cattaneo , B. Chadaj , M. Charles , Ph. Charpentier , J. Cheng , N. Chiapolini , A. Chlopik , J. Christiansen , P. Ciambrone , 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 , A. Comerma-Montells , F. Constantin , G. Conti , A. Contu , P. Cooke , M. Coombes , B. Corajod , G. Corti , G. A. Cowan , R. Currie , B. D'Almagne , C. D'Ambrosio , I. D'Antone , W. Da Silva , E. Dane' , 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 , G. Decreuse , H. Degaudenzi , M. Deissenroth , L. Del Buono , C. J. Densham , C. Deplano , O. Deschamps , F. Dettori , J. Dickens , H. Dijkstra , M. Dima , S. Donleavy , P. Dornan , D. Dossett , A. Dovbnya , R. Dumps , F. Dupertuis , L. Dwyer , 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 , G. Felici , V. Fernandez Albor , M. Ferro-Luzzi , S. Filippov , C. Fitzpatrick , W. Flegel , F. Fontanelli , C. Forti , R. Forty , C. Fournier , B. Franek , 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 , L. Garrido , D. Gascon , C. Gaspar , A. Gaspar De Valenzuela Cue , J. Gassner , N. Gauvin , P. Gavillet , M. Gersabeck , T. Gershon , Ph. Ghez , V. Gibson , V. V. Gligorov , C. Göbel , D. Golubkov , A. Golutvin , A. Gomes , G. Gong , H. Gong , H. Gordon , M. Grabalosa Gándara , V. Gracco , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , G. Graziani , A. Grecu , S. Gregson , G. Guerrer , B. Gui , E. Gushchin , Yu. Guz , Z. Guzik , 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 , H. J. Hilke , W. Hofmann , K. Holubyev , P. Hopchev , W. Hulsbergen , P. Hunt , T. Huse , R. S. Huston , D. Hutchcroft , F. Iacoangeli , V. Iakovenko , C. Iglesias Escudero , C. Ilgner , P. Ilten , J. Imong , R. Jacobsson , M. Jahjah Hussein , O. Jamet , E. Jans , F. Jansen , P. Jaton , B. Jean-Marie , M. John , D. Johnson , C. R. Jones , B. Jost , F. Kapusta , T. M. Karbach , A. Kashchuk , S. Katvars , J. Keaveney , U. Kerzel , T. Ketel , A. Keune , S. Khalil , B. Khanji , Y. M. Kim , M. Knecht , S. Koblitz , A. Konoplyannikov , P. Koppenburg , M. Korolev , A. Kozlinskiy , L. Kravchuk , R. Kristic , G. Krocker , P. Krokovny , F. Kruse , K. Kruzelecki , M. Kucharczyk , I. Kudryashov , 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. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , F. Lehner , M. Lenzi , O. Leroy , T. Lesiak , L. Li , Y. Y. Li , L. Li Gioi , J. Libby , M. Lieng , R. Lindner , S. Lindsay , C. Linn , B. Liu , G. Liu , S. Löchner , J. H. Lopes , E. Lopez Asamar , N. Lopez-March , P. Loveridge , 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 , D. Martinez Santos , A. Massafferri , Z. Mathe , C. Matteuzzi , V. Matveev , E. Maurice , B. Maynard , A. Mazurov , G. McGregor , R. McNulty , C. Mclean , M. Merk , J. Merkel , M. Merkin , R. Messi , S. Miglioranzi , M. -N. Minard , G. Moine , S. Monteil , D. Moran , J. Morant , P. Morawski , J. V. Morris , J. Moscicki , 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 , A. Nawrot , M. Nedos , M. Needham , N. Neufeld , P. Neustroev , M. Nicol , L. Nicolas , S. Nies , V. Niess , N. Nikitin , A. Noor , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , O. Okhrimenko , R. Oldeman , M. Orlandea , A. Ostankov , B. Pal , J. Palacios , M. Palutan , J. Panman , A. Papadelis , A. Papanestis , M. Pappagallo , C. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , S. K. Paterson , G. N. Patrick , C. Patrignani , E. Pauna , C. Pauna , C. Pavel , A. Pazos Alvarez , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , D. L. Perego , E. Perez Trigo , A. Pérez-Calero Yzquierdo , P. Perret , G. Pessina , A. Petrella , A. Petrolini , E. Picatoste Olloqui , B. Pie Valls , D. Piedigrossi , B. Pietrzyk , D. Pinci , S. Playfer , M. Plo Casasus , M. Poli-Lener , G. Polok , A. Poluektov , E. Polycarpo , D. Popov , B. Popovici , S. Poss , C. Potterat , A. Powell , S. Pozzi , T. du Pree , V. Pugatch , A. Puig Navarro , W. Qian , J. H. Rademacker , B. Rakotomiaramanana , I. Raniuk , G. Raven , S. Redford , W. Reece , A. C. dos Reis , S. Ricciardi , J. Riera , K. Rinnert , D. A. Roa Romero , P. Robbe , E. Rodrigues , F. Rodrigues , C. Rodriguez Cobo , P. Rodriguez Perez , G. J. Rogers , V. Romanovsky , E. Rondan Sanabria , M. Rosello , J. Rouvinet , L. Roy , T. Ruf , H. Ruiz , C. Rummel , V. Rusinov , G. Sabatino , J. J. Saborido Silva , N. Sagidova , P. Sail , B. Saitta , T. Sakhelashvili , C. Salzmann , A. Sambade Varela , M. Sannino , R. Santacesaria , R. Santinelli , E. Santovetti , M. Sapunov , A. Sarti , C. Satriano , A. Satta , T. Savidge , M. Savrie , D. Savrina , P. Schaack , M. Schiller , S. Schleich , M. Schmelling , B. Schmidt , O. Schneider , T. Schneider , A. Schopper , M. -H. Schune , R. Schwemmer , A. Sciubba , M. Seco , A. Semennikov , K. Senderowska , N. Serra , J. Serrano , B. Shao , M. Shapkin , I. Shapoval , P. Shatalov , Y. Shcheglov , T. Shears , L. Shekhtman , V. Shevchenko , A. Shires , S. Sigurdsson , E. Simioni , H. P. Skottowe , T. Skwarnicki , N. Smale , A. Smith , A. C. Smith , N. A. Smith , K. Sobczak , F. J. P. Soler , A. Solomin , P. Somogy , F. Soomro , B. Souza De Paula , B. Spaan , A. Sparkes , E. Spiridenkov , P. Spradlin , A. Srednicki , F. Stagni , S. Stahl , S. Steiner , O. Steinkamp , O. Stenyakin , S. Stoica , S. Stone , B. Storaci , U. Straumann , N. Styles , M. Szczekowski , P. Szczypka , T. Szumlak , S. T'Jampens , E. Tarkovskiy , E. Teodorescu , H. Terrier , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , S. Topp-Joergensen , M. T. Tran , S. Traynor , U. Trunk , A. Tsaregorodtsev , N. Tuning , A. Ukleja , O. Ullaland , 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. Volyanskyy , 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 , M. L. Woodward , S. A. Wotton , K. Wyllie , Y. Xie , F. Xing , Z. Yang , G. Ybeles Smit , R. Young , O. Yushchenko , M. Zeng , L. Zhang , Y. Zhang , A. Zhelezov , E. Zverev

Hadronic cross sections are important ingredients in many of the ongoing research methods in high-energy nuclear physics, and it is always important to measure and/or calculate the probabilities of different types of reactions. In heavy-ion…

Nuclear Theory · Physics 2021-02-25 Gábor Balassa , György Wolf

The study of b-hadrons made possible a great number of benchmark results in flavour physics. In recent years a lot of effort in understanding their dynamics has been done. These studies can represent a possible avenue for the discovery of…

High Energy Physics - Experiment · Physics 2012-09-04 F. Ruffini

The fragmentation functions for $c$ or $\bar{b}$ quark to $B_c$ or $B_c^*$ meson are derived up to QCD next-to-leading order (NLO). They are further computed numerically and presented in figures precisely. In order to reach a higher…

High Energy Physics - Phenomenology · Physics 2020-01-01 Xu-Chang Zheng , Chao-Hsi Chang , Tai-Fu Feng , Xing-Gang Wu

The properties of the $B_c$-meson family ($c\bar b$) are still not well determined experimentally because the specific mechanisms of formation and decay remain poorly understood. Unlike heavy quarkonia, i.e. the hidden heavy quark-antiquark…

High Energy Physics - Phenomenology · Physics 2022-10-05 B. Martín-González , P. G. Ortega , D. R. Entem , F. Fernández , J. Segovia

The total photoabsorption cross section on the nucleon is studied using nondiagonal GVDM. Vector meson-nucleon scattering amplitudes are calculated in two-gluon exchange approximation of QCD. The off-diagonal transitions of diffraction…

High Energy Physics - Phenomenology · Physics 2007-05-23 E. V. Bugaev , B. V. Mangazeev

The ratios of the B$_\mathrm{c}$(2S)$^+$ to B$_\mathrm{c}^+$, B$_\mathrm{c}^*$(2S)$^+$ to B$_\mathrm{c}^+$, and B$_\mathrm{c}^*$(2S)$^+$ to B$_\mathrm{c}$(2S)$^+$ production cross sections are measured in proton-proton collisions at…

High Energy Physics - Experiment · Physics 2020-11-25 CMS Collaboration

Quark and lepton flavor signals are studied in four supersymmetric models, namely the minimal supergravity model, the minimal supersymmetric standard model with right-handed neutrinos, SU(5) supersymmetric grand unified theory with…

High Energy Physics - Phenomenology · Physics 2008-11-26 Toru Goto , Yasuhiro Okada , Tetsuo Shindou , Minoru Tanaka

Neutral $B$ meson mixing matrix elements and $B$ meson decay constants are calculated. Static approximation is used for $b$ quark and domain-wall fermion formalism is employed for light quarks. The calculations are carried out on $2+1$…

High Energy Physics - Lattice · Physics 2015-06-30 Yasumichi Aoki , Tomomi Ishikawa , Taku Izubuchi , Christoph Lehner , Amarjit Soni

A combined expansion in the number of QCD colors 1/N_c and SU(3) flavor breaking parameter epsilon has long been known to provide an excellent accounting for the mass spectrum of the lightest spin-1/2, 3/2 baryons when the quarks are taken…

High Energy Physics - Phenomenology · Physics 2013-05-30 Aleksey Cherman , Thomas D. Cohen , Richard F. Lebed

A diagrammatic approach to quark exchange processes in meson-meson scattering is applied to the case of inelastic reactions of the type $(Q\barQ)+(q\barq)\rightarrow (Q\barq) + (q\barQ)$, where $Q$ and $q$ refer to heavy and light quarks,…

High Energy Physics - Phenomenology · Physics 2009-09-25 K. Martins , D. Blaschke , E. Quack

The inclusive direct and cascade semileptonic branching ratios of the b quark were measured from a fit to the lepton momentum spectrum in the B-hadron rest frame, exploiting the charge correlation between the lepton and the heavy meson. The…

High Energy Physics - Experiment · Physics 2007-05-23 Martino Margoni

We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-leading logarithmic approximation using the nonrelativistic renormalization group. We predict the mass difference of the vector and…

High Energy Physics - Phenomenology · Physics 2019-01-03 A. A. Penin , A. Pineda , V. A. Smirnov , M. Steinhauser

We derive QCD light-cone sum rules for the hadronic matrix elements of the heavy baryon transitions to nucleon. In the correlation functions the $\Lambda_c,\Sigma_c$ and $\Lambda_b$ -baryons are interpolated by three-quark currents and the…

High Energy Physics - Phenomenology · Physics 2015-05-30 A. Khodjamirian , Ch. Klein , Th. Mannel , Y. -M. Wang

The uncertainties of the Standard Model prediction of the anomalous magnetic moment of the muon are currently completely dominated by hadronic contributions. The largest contribution is due to the hadronic vacuum polarization. Hadronic…

High Energy Physics - Experiment · Physics 2018-12-05 C. F. Redmer
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