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Related papers: Upper Limit on the Decay K+ --> e+ nu mu+ mu-

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A preliminary measurement of the branching fraction of the tau- -> 3h-2h+nu decay (h= pi, K$) with the BaBar detector is found to be {8.52 +/- 0.09 +/- 0.40} x 10E-4, where the first error is statistical and the second is systematic. The…

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

From a data sample of 29058 $\tau^\pm\to\pi^\pm\pi^+\pi^-\pi^0\nu_\tau$ decays observed in the CLEO detector we derive a 95% confidence upper limit on the tau neutrino mass of 28 MeV.

High Energy Physics - Experiment · Physics 2010-04-08 M. Athanas

We report on a search for the flavor-changing neutral current decays B^+ -> mu^+ mu^- K^+ and B^0 -> mu^+ mu^- K^{*0} using 88 pb^{-1} of data from p-pbar collisions at \sqrt{s}=1.8 TeV, collected with the Collider Detector at Fermilab.…

High Energy Physics - Experiment · Physics 2012-08-27 CDF Collaboration

Using 15.1 pb^{-1} of data collected by CMD-2 in the phi-meson energy range, the branching ratios of the following conversion decays have been measured: B(\phi\to\eta e^+e^-) = (1.14\pm0.10\pm0.06)\cdot10^{-4}, B(\eta\to e^+e^-\gamma) =…

High Energy Physics - Experiment · Physics 2008-11-26 2 collaboration

We test whether or not the tau lepton manifests the same couplings as the mu lepton by investigating the relative decay rates in purely leptonic D+ meson decays. Specifically, we place the first upper limit on the ratio R=Gamma(D+ -> tau+…

High Energy Physics - Experiment · Physics 2010-04-08 P. Rubin , CLEO Collaboration

We have searched a sample of 9.6 million BBbar events for the flavor-changing neutral current decays B -> K l^+ l^- and B -> K^*(892) l^+ l^-. We subject the latter decay to the requirement that the dilepton mass exceed 0.5 GeV. There is no…

High Energy Physics - Experiment · Physics 2010-05-28 S. Anderson , CLEO Collaboration

The decay branching fractions of the three narrow Upsilon resonances to mu+mu- have been measured by analyzing about 4.3 1/fb e+e- data collected in the vicinity of the resonances with the CLEO III detector. The branching fraction B(Y(1S)…

High Energy Physics - Experiment · Physics 2019-08-14 G. S. Adams

We measure the branching fraction of the radiative B- decay B(B- -> phi K- gamma) = (3.46 +/- 0.57^{+0.39}_{-0.37}) 10^-6, and set an upper limit on the radiative B0 decay B(B0 -> phi K0 gamma) < 2.71 10^-6 at 90% confidence level. We also…

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

We have observed the decays B-->phi K and phi K^* in a sample of over 45 million B mesons collected with the BABAR detector at the PEP-II collider. The measured branching fractions are BF(B^+ --> phi K^+) = (7.7^{+1.6}_{-1.4}+/- 0.8) x…

High Energy Physics - Experiment · Physics 2010-05-28 B. Aubert , BABAR Collaboration

We search for the rare leptonic decay B+ --> tau+ nu_tau in a sample of 232x10^6 BBbar pairs collected with the BABAR detector at the SLAC PEP-II B-Factory. Signal events are selected by examining the properties of the B meson recoiling…

High Energy Physics - Experiment · Physics 2010-03-19 The BABAR Collaboration , B. Aubert

A search for the decay of the tau lepton to five charged and two neutral pions is performed using data collected by the BABAR detector at the PEP-II asymmetric-energy e+e- collider. The analysis uses 232 fb-1 of data at center-of-mass…

High Energy Physics - Experiment · Physics 2010-03-19 The BABAR Collaboration , B. Aubert

We present results of searches for B-meson decays to K+ pi- pi+ with the BaBar detector. With a data sample of 61.6 million BBbar pairs, we measure the branching fractions and 90% confidence-level upper limits averaged over charge-conjugate…

High Energy Physics - Experiment · Physics 2008-11-26 B. Aubert

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

The decay $K_L \to \gamma \nu \bar{\nu}$ is investigated beyond the standard model. Interestingly, the upper limit of the CP-conserving and CP-violating branching ratios of the decay, induced from the possible extensions of the standard…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ji-Hao Jiang , Dao-Neng Gao , Mu-Lin Yan

An additional event near the upper kinematic limit for K+ to pi+ nu nubar has been observed by Experiment E949 at Brookhaven National Laboratory. Combining previously reported and new data, the branching ratio is B(K+ to pi+ nu nubar)= 1.47…

High Energy Physics - Experiment · Physics 2008-11-26 E949 Collaboration , A. V. Artamonov

We search for b to s\mu^+\mu^- transitions in B meson (B^+, B^0, or B^0_s) decays with 924pb^{-1} of p pbar collisions at sqrt(s)=1.96 TeV collected with the CDF II detector at the Fermilab Tevatron. We find excesses with significances of…

High Energy Physics - Experiment · Physics 2010-05-12 CDF Collaboration , T. Aaltonen

We have performed a search for Bs-->mu+mu- and Bd-->mu+mu- decays in ppbar collisions at sqrt(s) = 1.96TeV using 2fb-1 of integrated luminosity collected by the CDF II detector at the Fermilab Tevatron Collider. The observed number of Bs…

High Energy Physics - Experiment · Physics 2010-05-12 CDF Collaboration , T. Aaltonen

Using a 13.7 fb-1 data sample collected with the CLEO II and II.V detectors, we report new branching fraction measurements for two Cabibbo-suppressed decay modes of the D+ meson: BR(D+ -> pi+ pi0) = (1.31 +/- 0.17 +/- 0.09 +/- 0.09) x…

High Energy Physics - Experiment · Physics 2010-04-08 K. Arms

The reaction pd->3He eta at threshold was used to provide a clean source of eta mesons for decay studies with the WASA detector at CELSIUS. The branching ratio of the decay eta->pi+pi-e+e- is measured to be (4.3+/-1.3+/-0.4)x10^-4.