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Related papers: B_{s1}(5830) and B_{s2}^*(5840)

200 papers

Excited $B$-mesons have been observed by the D0, CDF, LHCb and CMS experiments. We use the predictions of the relativized quark model to make quark model spectroscopic assignments for these states. We identify the $B_2^*(5747)$ and…

High Energy Physics - Phenomenology · Physics 2019-06-26 Stephen Godfrey , Kenneth Moats

Based on a data sample of an integrated luminosity of 57.4 fb-1 at the Upsilon(4S) resonance taken with the BaBar detector using the SLAC PEP-II asymmetric-energy $B$-Factory, hadronic decays of B meson with the final states D(*) and three…

High Energy Physics - Experiment · Physics 2007-05-23 H. W. Zhao

The measurements of B_s mesons and b baryons advanced greatly in the past year. The ground state b baryon Xi_b^0 was observed for the first time; numerous decay modes of the B_s^0 and b baryons were newly seen; measurements of CP violation…

High Energy Physics - Experiment · Physics 2012-01-24 R. F. Harr

We have searched for two-body charmless hadronic decays of $B$ mesons. Final states include $\pi\pi$, $K \pi$, and $KK$ with both charged and neutral kaons and pions; $\pi\rho$, $K \rho$, and $K^*\pi$; and $K\phi$, $ K^*\phi$, and…

High Energy Physics - Experiment · Physics 2008-11-26 CLEO Collaboration , D. M. Asner et al

Goldstone boson decays of P-wave $D_s^{**}$ mesons are studied within the framework of Heavy Hadron Chiral Perturbation Theory. We first analyze the simplest single kaon decays of these strange charmed mesons. We derive a model independent…

High Energy Physics - Phenomenology · Physics 2009-10-22 Peter Cho , Sandip P. Trivedi

Using special linear combinations of finite energy sum rules which minimize the contribution of the unknown continuum spectral function, we compute the decay constants of the pseudoscalar mesons B and B_s. In the computation, we employ the…

High Energy Physics - Phenomenology · Physics 2011-01-27 J. Bordes , J. Peñarrocha , K. Schilcher

A search is presented for single production of heavy vector-like quarks (B) that decay to a Higgs boson and a b quark, with the Higgs boson decaying to a highly boosted $\mathrm{b\overline{b}}$ pair reconstructed as a single collimated jet.…

High Energy Physics - Experiment · Physics 2018-06-18 CMS Collaboration

In the framework of the coupled channel model the mass shifts of the $P$--wave excitations of $D_s$ and $B_s$ mesons have been calculated. The corresponding coupling to $DK$ and $BK$ channels is provided by the effective chiral Lagrangian…

High Energy Physics - Phenomenology · Physics 2008-11-17 A. M. Badalian , Yu. A. Simonov , M. A. Trusov

The $\Delta S = 2$ transition $b \to s s \bar d$ is extremely small in the standard model, proceeding only via box diagrams. Such decays are thus an appropriate ground for searching new physics. We present a study of several two-body and…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Fajfer , J. Kamenik , P. Singer

We report the observation of two narrow structures in the mass spectra of the pi+-Y(nS) (n=1,2,3) and pi+-hb(mP)(m$ (m=1,2) pairs that are produced in association with a single charged pion in Y(5S) decays. The measured masses and widths of…

High Energy Physics - Experiment · Physics 2013-05-30 the Belle Collaboration

The $B_c$ meson, a unique bound state comprising of two open heavy flavors, charm and bottom, offers a rich avenue for probing the predictions of the Next Decade - Standard Model (ND-SM) physics properties due to its heavy mass. With recent…

High Energy Physics - Phenomenology · Physics 2024-11-19 Sonali Patnaik

The two B^0 decay processes B^0 --> D^{*-}pi^+ and B^0 --> D^{*-}l^+nu have been studied by means of a partial reconstruction technique using a data sample collected with the BABAR detector at the PEP-II storage ring. To increase…

High Energy Physics - Experiment · Physics 2007-05-23 The BABAR Collaboration , B. Aubert

The measured masses and strong decays of $\Lambda_b(6146)^0$ and $\Lambda_b(6152)^0$ required us to decode them as the 1$D$ excited states with $J^P=3/2^+$ and $J^P=5/2^+$, respectively. Under the suggested assignment, the masses and total…

High Energy Physics - Phenomenology · Physics 2019-11-28 Bing Chen , Si-Qiang Luo , Xiang Liu , Takayuki Matsuki

A survey of the experimental, phenomenological, and theoretical status of the new heavy mesons is presented. States discussed are the $B_c$, $h_c$, $\eta_c'$, $D_s(2317)$, $D_s(2460)$, X(3872), X(3940), Y(3940), Z(3930), and Y(4260). Quark…

High Energy Physics - Phenomenology · Physics 2008-11-26 Eric S. Swanson

Using QCD sum rules and chiral SU(3) model, we investigate the effect of temperature, density, strangeness fraction and isospin asymmetric parameter on the shift in masses and decay constants of the pseudoscalar $D$ and $B$ meson in…

High Energy Physics - Phenomenology · Physics 2017-08-23 Rahul Chhabra , Arvind Kumar

The new mesons $X(3940)$ and $X(4160)$ have been found by Belle Collaboration in the processes $e^+e^-\to J/\psi D^{(*)}\bar D^{(*)}$. Considering $X(3940)$ and $X(4160)$ as $\eta_c(3S)$ and $\eta_c(4S)$ states, the two-body open charm…

High Energy Physics - Phenomenology · Physics 2017-03-08 Zhi-Hui Wang , Yi Zhang , Libo Jiang , Tian-Hong Wang , Yue Jiang , Guo-Li Wang

The decays of $B$ mesons to two-body hadronic final states are analyzed within the context of broken flavor SU(3) symmetry, extending a previous analysis involving pairs of light pseudoscalars to decays involving one or two charmed quarks…

High Energy Physics - Phenomenology · Physics 2010-11-01 Michael Gronau , Oscar F. Hernandez , David London , Jonathan L. Rosner

In this work, we present a systematic study of the observed isoscalar tensor $f_2$ states. With the detailed analysis of the mass spectrum and calculation of the $f_2$ two-body strong decays, we extract information of their underly…

High Energy Physics - Phenomenology · Physics 2012-09-27 Zao-Chen Ye , Xiao Wang , Xiang Liu , Qiang Zhao

A search for the decays Bs-->mumu and Bd-->mumu is performed with about 37 pb^{-1} of pp collisions at sqrt{s} = 7 TeV collected by the LHCb experiment at the Large Hadron Collider at CERN. The observed numbers of events are consistent with…

High Energy Physics - Experiment · Physics 2015-03-19 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 , 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 , 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 , Ch. Elsasser , D. G. d'Enterria , D. Esperante Pereira , L. Estève , A. Falabella , 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 , 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 , 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. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , S. K. Paterson , G. N. Patrick , C. Patrignani , C. Pavel -Nicorescu , A. Pazos Alvarez , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , D. L. Perego , E. Perez Trigo , A. Pérez-Calero Yzquierdo , P. Perret , A. Petrella , A. Petrolini , B. Pie Valls , B. Pietrzyk , D. Pinci , R. Plackett , S. Playfer , M. Plo Casasus , G. Polok , A. Poluektov , E. Polycarpo , D. Popov , B. Popovici , C. Potterat , A. Powell , 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 , K. Rinnert , D. A. Roa Romero , P. Robbe , E. Rodrigues , F. Rodrigues , C. Rodriguez Cobo , P. Rodriguez Perez , G. J. Rogers , V. Romanovsky , J. Rouvinet , T. Ruf , H. Ruiz , G. Sabatino , J. J. Saborido Silva , N. Sagidova , P. Sail , B. Saitta , C. Salzmann , A. Sambade Varela , M. Sannino , R. Santacesaria , R. Santinelli , E. Santovetti , M. Sapunov , A. Sarti , C. Satriano , A. Satta , M. Savrie , D. Savrina , P. Schaack , M. Schiller , S. Schleich , M. Schmelling , B. Schmidt , O. 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 , O. Shevchenko , V. Shevchenko , A. Shires , E. Simioni , H. P. Skottowe , T. Skwarnicki , A. C. 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 , F. Stagni , O. Steinkamp , O. Stenyakin , S. Stoica , S. Stone , B. Storaci , U. Straumann , N. Styles , M. Szczekowski , P. Szczypka , T Szumlak , S. T'Jampens , V. Talanov , E. Teodorescu , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , S. Topp-Joergensen , M. T. Tran , A. Tsaregorodtsev , N. 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 , 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

Different from the previous treatment in a two-body framework, we introduce the dimeson distribution amplitudes (DAs) to describe the strong dynamics between the S-wave resonances $a_0(980, 1450)$ and the $K\bar K (\pi\eta)$ pair, where the…

High Energy Physics - Phenomenology · Physics 2024-11-07 Si-Yang Wang , Zhi-Qing Zhang , Zhi-Jie Sun , Jian Chai , Peng Li