University of Birmingham First Observation of the Decay Bs0 K-+ and a Measurement of |Vub | / |Vcb |

C. A. Barajas,M. Chefdeville,C. Chen,S. Chen,A. Chernov,S. Chitic,V. Chobanova,S. Cholak,M. Chrzaszcz,A. Chubykin,V. Chulikov,P. Ciambrone,M. Cicala,X. Vidal,G. Ciezarek,P. Clarke,M. Clemencic,H. Cliff,J. Closier,J. Cobbledick,V. Coco,J. Coelho,J. Cogan,E. Cogneras,L. Cojocariu,P. Collins,T. Colombo,L. Congedo,A. Contu,N. Cooke,G. Coombs,G. Corti, C. Sobral,B. Couturier,D. Craik,J. Crkovská,M. C. Torres,R. Currie,C. L. Silva,E. Dall, Occo,J. Dalseno, D. C, Ambrosio,A. Danilina,A. Davis, O. Francisco,K. Bruyn,S. Capua,M. Cian,J. Miranda,L. Paula,M. Serio, D. Simone, P. Simone,J. A. Vries,C. Dean,W. Dean,D. Decamp,L. Buono,B. Delaney,H. Dembinski,A. Dendek,V. Denysenko,D. Derkach,O. Deschamps,F. Desse,F. Dettori,B. Dey,P. Nezza,S. Didenko,L. D. Maronas,H. Dijkstra,V. Dobishuk,A. M. Donohoe,F. Dordei,A. Reis,L. Douglas,A. Dovbnya,A. Downes,K. Dreimanis,M. Dudek,L. Dufour,V. Duk, P. Durante,J. Durham,D. Dutta,M. Dziewiecki,A. Dziurda,A. Dzyuba,S. Easo,U. Egede,V. Egorychev, S. Eidelman,S. Eisenhardt,L. Eklund,S. Ely,A. Ene,E. Epple,S. Escher,J. Eschle,S. Esen,T. Evans,A. Falabella,J. Fan,Y. Fan,B. Fang,N. Farley,S. Farry,D. Fazzini,P. Fedin,M. Feo,P. F. Declara,A. F. Prieto,F. Ferrari,L. Lopes,F. Rodrigues,S. F. Sole,M. Ferrillo,M. Ferro-Luzzi,Sergey Filippov,R. Fini,M. Fiorini,M. Firlej,C. Fitzpatrick,T. Fiutowski,F. Fleuret,M. Fontana,F. Fontanelli,R. Forty,V. F. Lima,M. Sevilla,M. Frank,E. Franzoso,G. Frau,C. Frei,D. Friday,Q. Fuehring,W. Funk,E. Gabriel,T. Gaintseva,A. G. Torreira,D. Galli,S. Gambetta,Y. Gan,M. Gandelman,P. Gandini,Y. Gao,M. Garau,L. Martin,P. Moreno,J. G. Pardiñas,B. G. Plana,F. A. G. Rosales,L. Garrido,C. Gaspar,R. Geertsema,D. Gerick,L. L. Gerken,E. Gersabeck,M. Gersabeck,T. Gershon,D. Gerstel,P. Ghez,V. Gibson,M. Giovannetti,A. Gioventù,P. G. Gironell,L. Giubega,C. Giugliano,K. Gizdov,E. Gkougkousis,V. Gligorov,C. Göbel,E. Golobardes,D. Golubkov,A. Golutvin,A. Gomes,S. Fernandez,F. G. Abrantes,M. Goncerz,G. Gong,P. Gorbounov,I. Gorelov,C. Gotti,J. P. Grabowski,R. Diaz,T. Grammatico,L. Cardoso,E. Grauges,E. Graverini,G. Graziani,A. Grecu,L. M. Greeven,P. Griffith,L. Grillo,S. Gromov,B. Cazon,C. Gu,Marco Guarise,P. Günther,E. Gushchin,A. Guth,Y. Guz,T. Gys,T. Hadavizadeh,G. Haefeli, C. Haen,J. Haimberger,P. Hamilton,Q. Han,X. Han,S. Hansmann-Menzemer,N. Harnew,T. Harrison,C. Hasse,M. Hecker,K. Heijhoff,K. Heinicke,A. Hennequin,K. Hennessy,L. Henry,J. Heuel,A. Hicheur,M. Hilton,S. Hollitt,W. Huang,W. Hulsbergen,R. Hunter,M. Hushchyn,D. Hutchcroft,D. Hynds, P. Ibis,M. Idzik, D. Ilin,P. Ilten,A. Inglessi,A. Ishteev,K. Ivshin,R. Jacobsson,S. Jakobsen,E. Jans,B. Jashal,A. Jawahery,Vukan Jevtic,M. Jeżabek,F. Jiang,M. John,D. Johnson,C. R. Jones,T. Jones,B. Jost,N. Jurik,S. Kandybei,Y. Kang,M. Karacson,M. Karpov,N. Kazeev, F. Keizer,M. Kenzie,T. Ketel,B. Khanji, A. Kharisova,S. Kholodenko,T. Kirn, O. Kitouni,S. Klaver,S. Koliiev,A. Kondybayeva, A. Konoplyannikov,P. Kopciewicz, R. Kopecná,P. Koppenburg, I. Kostiuk, O. Kot,S. Kotriakhova,P. Kravchenko,L. Kravchuk,M. Kreps, F. Kress,S. Kretzschmar,P. Krokovny,W. Krzemień,W. Kucewicz,V. Kudryavtsev,T. Kvaratskheliya,D. Lacarrere,G. Lafferty,A. Lai, A. Lampis, D. Lancierini,O. Lantwin,T. Latham, F. Lazzari,R. Gac, A. Leflat, S. Legotin,O. Leroy,T. Lesiak, B. Leverington,V. Lisovskyi,R. Litvinov,G. Liu,H. Liu,J. L. Castro,I. Longstaff,J. Lopes, G. Loustau, G. Lovell,Y. Lu,D. Lucchesi,S. Luchuk,M. Martinez,V. Lukashenko, Yongde Luo,A. Lupato,E. Luppi,A. Lusiani,X. Lyu, S. Maccolini,F. Maciuc,V. Macko,O. Madejczyk,L. R. M. Mohan,O. Maev,A. Maevskiy, D. Maisuzenko,S. Malde, B. Malecki,A. Malinin,T. Maltsev,G. Manca,G. Mancinelli, R. M. Escalero, D. Manuzzi,J. Maratas,S. Mariani

semanticscholar(2021)

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摘要
The first observation of the suppressed semileptonic B 0 s → K − μ þ ν μ decay is reported. Using a data sample recorded in pp collisions in 2012 with the LHCb detector, corresponding to an integrated luminosity of 2 fb − 1 , the branching fraction B ð B 0 s → K − μ þ ν μ Þ is measured to be ½ 1 . 06 (cid:2) 0 . 05 ð stat Þ(cid:2) 0 . 08 ð syst Þ(cid:3) × 10 − 4 , where the first uncertainty is statistical and the second one represents the combined systematic uncertainties. The decay B 0 s → D − s μ þ ν μ , where D − s is reconstructed in the final state K þ K − π − , is used as a normalization channel to minimize the experimental systematic uncertainty. Theoretical calculations on the form factors of the B 0 s → K − and B 0 s → D − s transitions are employed to determine the ratio of the Cabibbo-Kobayashi-Maskawa matrix elements j V ub j = j V cb j at low and high B 0 s → K − momentum transfer.
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