학술논문

Observation of the decay B¯s0→ψ(2S)K+π−
Document Type
article
Author
R. AaijB. AdevaM. AdinolfiA. AffolderZ. AjaltouniS. AkarJ. AlbrechtF. AlessioM. AlexanderS. AliG. AlkhazovP. Alvarez CartelleA.A. Alves JrS. AmatoS. AmerioY. AmhisL. AnL. AnderliniJ. AndersonM. AndreottiJ.E. AndrewsR.B. ApplebyO. Aquines GutierrezF. ArchilliA. ArtamonovM. ArtusoE. AslanidesG. AuriemmaM. BaalouchS. BachmannJ.J. BackA. BadalovC. BaessoW. BaldiniR.J. BarlowC. BarschelS. BarsukW. BarterV. BatozskayaV. BattistaA. BayL. BeaucourtJ. BeddowF. BedeschiI. BediagaL.J. BelI. BelyaevE. Ben-HaimG. BencivenniS. BensonJ. BentonA. BerezhnoyR. BernetA. BertolinM.-O. BettlerM. van BeuzekomA. BienS. BifaniT. BirdA. BizzetiT. BlakeF. BlancJ. BlouwS. BluskV. BocciA. BondarN. BondarW. BoniventoS. BorghiM. BorsatoT.J.V. BowcockE. BowenC. BozziS. BraunD. BrettM. BritschT. BrittonJ. BrodzickaN.H. BrookA. BurscheJ. BuytaertS. CadedduR. CalabreseM. CalviM. Calvo GomezP. CampanaD. Campora PerezL. CapriottiA. CarboneG. CarboniR. CardinaleA. CardiniP. CarnitiL. CarsonK. Carvalho AkibaR. Casanova MohrG. CasseL. CassinaL. Castillo GarciaM. CattaneoCh. CauetG. CavalleroR. CenciM. CharlesPh. CharpentierM. ChefdevilleS. ChenS.-F. CheungN. ChiapoliniM. ChrzaszczX. Cid VidalG. CiezarekP.E.L. ClarkeM. ClemencicH.V. CliffJ. ClosierV. CocoJ. CoganE. CognerasV. CogoniL. CojocariuG. CollazuolP. CollinsA. Comerma-MontellsA. ContuA. CookM. CoombesS. CoquereauG. CortiM. CorvoI. CountsB. CouturierG.A. CowanD.C. CraikA.C. CrocombeM. Cruz TorresS. CunliffeR. CurrieC. D'AmbrosioJ. DalsenoP.N.Y. DavidA. DavisK. De BruynS. De CapuaM. De CianJ.M. De MirandaL. De PaulaW. De SilvaP. De SimoneC.-T. DeanD. DecampM. DeckenhoffL. Del BuonoN. DéléageD. DerkachO. DeschampsF. DettoriB. DeyA. Di CantoF. Di RuscioH. DijkstraS. DonleavyF. DordeiM. DorigoA. Dosil SuárezD. DossettA. DovbnyaK. DreimanisG. DujanyF. DupertuisP. DuranteR. DzhelyadinA. DziurdaA. DzyubaS. EasoU. EgedeV. EgorychevS. EidelmanS. EisenhardtU. EitschbergerR. EkelhofL. EklundI. El RifaiCh. ElsasserS. ElyS. EsenH.M. EvansT. EvansA. FalabellaC. FärberC. FarinelliN. FarleyS. FarryR. FayD. FergusonV. Fernandez AlborF. FerrariF. Ferreira RodriguesM. Ferro-LuzziS. FilippovM. FioreM. FioriniM. FirlejC. FitzpatrickT. FiutowskiP. FolM. FontanaF. FontanelliR. FortyO. FranciscoM. FrankC. FreiM. FrosiniJ. FuE. FurfaroA. Gallas TorreiraD. GalliS. GalloriniS. GambettaM. GandelmanP. GandiniY. GaoJ. García PardiñasJ. GarofoliJ. Garra TicoL. GarridoD. GasconC. GasparU. GastaldiR. GauldL. GavardiG. GazzoniA. GeraciD. GerickE. GersabeckM. GersabeckT. GershonPh. GhezA. GianelleS. GianìV. GibsonL. GiubegaV.V. GligorovC. GöbelD. GolubkovA. GolutvinA. GomesC. GottiM. Grabalosa GándaraR. Graciani DiazL.A. Granado CardosoE. GraugésE. GraveriniG. GrazianiA. GrecuE. GreeningS. GregsonP. GriffithL. GrilloO. GrünbergB. GuiE. GushchinYu. GuzT. GysC. HadjivasiliouG. HaefeliC. HaenS.C. HainesS. HallB. HamiltonT. HampsonX. HanS. Hansmann-MenzemerN. HarnewS.T. HarnewJ. HarrisonJ. HeT. HeadV. HeijneK. HennessyP. HenrardL. HenryJ.A. Hernando MorataE. van HerwijnenM. HeßA. HicheurD. HillM. HoballahC. HombachW. HulsbergenT. HumairN. HussainD. HutchcroftD. HyndsM. IdzikP. IltenR. JacobssonA. JaegerJ. JalochaE. JansA. JawaheryF. JingM. JohnD. JohnsonC.R. JonesC. JoramB. JostN. JurikS. KandybeiW. KansoM. KaracsonT.M. KarbachS. KarodiaM. KelseyI.R. KenyonM. KenzieT. KetelB. KhanjiC. KhurewathanakulS. KlaverK. KlimaszewskiO. KochebinaM. KolpinI. KomarovR.F. KoopmanP. KoppenburgM. KorolevL. KravchukK. KreplinM. KrepsG. KrockerP. KrokovnyF. KruseW. KucewiczM. KucharczykV. KudryavtsevK. KurekT. KvaratskheliyaV.N. La ThiD. LacarrereG. LaffertyA. LaiD. LambertR.W. LambertG. LanfranchiC. LangenbruchB. LanghansT. LathamC. LazzeroniR. Le GacJ. van LeerdamJ.-P. LeesR. LefèvreA. LeflatJ. LefrançoisO. LeroyT. LesiakB. LeveringtonY. LiT. LikhomanenkoM. LilesR. LindnerC. LinnF. LionettoB. LiuS. LohnI. LongstaffJ.H. LopesP. LowdonD. LucchesiH. LuoA. LupatoE. LuppiO. LuptonF. MachefertF. MaciucO. MaevS. MaldeA. MalininG. MancaG. MancinelliP. ManningA. MapelliJ. MaratasJ.F. MarchandU. MarconiC. Marin BenitoP. MarinoR. MärkiJ. MarksG. MartellottiM. MartinelliD. Martinez SantosF. Martinez VidalD. Martins TostesA. MassafferriR. MatevA. MathadZ. MatheC. MatteuzziA. MauriB. MaurinA. MazurovM. McCannJ. McCarthyA. McNabR. McNultyB. MeadowsF. MeierM. MeissnerM. MerkD.A. MilanesM.-N. MinardD.S. MitzelJ. Molina RodriguezS. MonteilM. MorandinP. MorawskiA. MordàM.J. MorelloJ. MoronA.-B. MorrisR. MountainF. MuheimK. MüllerM. MussiniB. MusterP. NaikT. NakadaR. NandakumarI. NastevaM. NeedhamN. NeriS. NeubertN. NeufeldM. NeunerA.D. NguyenT.D. NguyenC. Nguyen-MauV. NiessR. NietN. NikitinT. NikodemA. NovoselovD.P. O'HanlonA. Oblakowska-MuchaV. ObraztsovS. OgilvyO. OkhrimenkoR. OldemanC.J.G. OnderwaterB. Osorio RodriguesJ.M. Otalora GoicocheaA. OttoP. OwenA. OyangurenA. PalanoF. PalomboM. PalutanJ. PanmanA. PapanestisM. PappagalloL.L. PappalardoC. ParkesG. PassalevaG.D. PatelM. PatelC. PatrignaniA. PearceA. PellegrinoG. PensoM. Pepe AltarelliS. PerazziniP. PerretL. PescatoreK. PetridisA. PetroliniE. Picatoste OlloquiB. PietrzykT. PilařD. PinciA. PistoneS. PlayferM. Plo CasasusT. PoikelaF. PolciA. PoluektovI. PolyakovE. PolycarpoA. PopovD. PopovB. PopoviciC. PotteratE. PriceJ.D. PriceJ. PrisciandaroA. PritchardC. ProuveV. PugatchA. Puig NavarroG. PunziW. QianR. QuaglianiB. RachwalJ.H. RademackerB. RakotomiaramananaM. RamaM.S. RangelI. RaniukN. RauschmayrG. RavenF. RediS. ReichertM.M. ReidA.C. dos ReisS. RicciardiS. RichardsM. RihlK. RinnertV. Rives MolinaP. RobbeA.B. RodriguesE. RodriguesJ.A. Rodriguez LopezP. Rodriguez PerezS. RoiserV. RomanovskyA. Romero VidalM. RotondoJ. RouvinetT. RufH. RuizP. Ruiz VallsJ.J. Saborido SilvaN. SagidovaP. SailB. SaittaV. Salustino GuimaraesC. Sanchez MayordomoB. Sanmartin SedesR. SantacesariaC. Santamarina RiosE. SantovettiA. SartiC. SatrianoA. SattaD.M. SaundersD. SavrinaM. SchillerH. SchindlerM. SchluppM. SchmellingB. SchmidtO. SchneiderA. SchopperM.-H. SchuneR. SchwemmerB. SciasciaA. SciubbaA. SemennikovI. SeppN. SerraJ. SerranoL. SestiniP. SeyfertM. ShapkinI. ShapovalY. ShcheglovT. ShearsL. ShekhtmanV. ShevchenkoA. ShiresR. Silva CoutinhoG. SimiM. SirendiN. SkidmoreI. SkillicornT. SkwarnickiN.A. SmithE. SmithJ. SmithM. SmithH. SnoekM.D. SokoloffF.J.P. SolerF. SoomroD. SouzaB. Souza De PaulaB. SpaanP. SpradlinS. SridharanF. StagniM. StahlS. StahlO. SteinkampO. StenyakinF. SterpkaS. StevensonS. StoicaS. StoneB. StoraciS. StrackaM. StraticiucU. StraumannR. StroiliL. SunW. SutcliffeK. SwientekS. SwientekV. SyropoulosM. SzczekowskiP. SzczypkaT. SzumlakS. T'JampensM. TeklishynG. TellariniF. TeubertC. ThomasE. ThomasJ. van TilburgV. TisserandM. TobinJ. ToddS. TolkL. TomassettiD. TonelliS. Topp-JoergensenN. TorrE. TournefierS. TourneurK. TrabelsiM.T. TranM. TreschA. TrisovicA. TsaregorodtsevP. TsopelasN. TuningA. UklejaA. UstyuzhaninU. UwerC. VaccaV. VagnoniG. ValentiA. VallierR. Vazquez GomezP. Vazquez RegueiroC. Vázquez SierraS. VecchiJ.J. VelthuisM. VeltriG. VenezianoM. VesterinenJ.V. Viana BarbosaB. ViaudD. VieiraM. Vieites DiazX. Vilasis-CardonaA. VollhardtD. VolyanskyyD. VoongA. VorobyevV. VorobyevC. VoßJ.A. de VriesR. WaldiC. WallaceR. WallaceJ. WalshS. WandernothJ. WangD.R. WardN.K. WatsonD. WebsdaleA. WeidenM. WhiteheadD. WiednerG. WilkinsonM. WilkinsonM. WilliamsM.P. WilliamsF.F. WilsonJ. WimberleyJ. WishahiW. WislickiM. WitekG. WormserS.A. WottonS. WrightK. WyllieY. XieZ. XuZ. YangX. YuanO. YushchenkoM. ZangoliM. ZavertyaevL. ZhangY. ZhangA. ZhelezovA. ZhokhovL. Zhong
Source
Physics Letters B, Vol 747, Iss C, Pp 484-494 (2015)
Subject
Physics
QC1-999
Language
English
ISSN
0370-2693
1873-2445
Abstract
The decay B¯s0→ψ(2S)K+π− is observed using a data set corresponding to an integrated luminosity of 3.0 fb−1 collected by the LHCb experiment in pp collisions at centre-of-mass energies of 7 and 8 TeV. The branching fraction relative to the B0→ψ(2S)K+π− decay mode is measured to beB(B¯s0→ψ(2S)K+π−)B(B0→ψ(2S)K+π−)=5.38±0.36(stat)±0.22(syst)±0.31(fs/fd)%, where fs/fd indicates the uncertainty due to the ratio of probabilities for a b quark to hadronise into a Bs0 or B0 meson. Using an amplitude analysis, the fraction of decays proceeding via an intermediate K⁎(892)0 meson is measured to be 0.645±0.049(stat)±0.049(syst) and its longitudinal polarisation fraction is 0.524±0.056(stat)±0.029(syst). The relative branching fraction for this component is determined to be B(B¯s0→ψ(2S)K⁎(892)0)B(B0→ψ(2S)K⁎(892)0)=5.58±0.57(stat)±0.40(syst)±0.32(fs/fd)%. In addition, the mass splitting between the Bs0 and B0 mesons is measured as M(Bs0)−M(B0)=87.45±0.44(stat)±0.09(syst) MeV/c2.