6533b831fe1ef96bd12990c5

RESEARCH PRODUCT

Production of excited beauty states in Z decays

Jordan NashH. VideauGunter QuastP. PayreI. SiotisGiuseppe IaselliAndré RosowskyJ.d. HansenJean-claude MontretU. StierlinP. HenrardH. DietlI. VideauS. L. CartwrightE. P. WhelanJiali LinA. M. StaceyC. GotzheinC. BoyerH. DuartePaul HankeP. ColasI. Ten HaveD.p.s. FergusonC. BenchoukK. JakobsR. AlemanyM. A. McneilM. I. WilliamsR. M. TurnbullS. WasserbaechG. SanguinettiM. Pepe-altarelliS. WernerA. CordierPierluigi CampanaM. MartinezRamon MiquelA. S. ThompsonS. BettariniR. XuFranco LigabueG. MannocchiXin WuR. FantechiF. CouraultD. KuhnR W AssmannC. N. BoothJ. JoussetMichael SchmittJ. P. LeesV. ChiarellaG. LütjensP. R. NortonJ. SommerF. MurtasSalvatore NuzzoG. BatignaniM. EdwardsM. N. MinardJ. J. WalshJd TurkJ. BoucrotM. CarpinelliP. RensingP. ColrainC. PadillaF. SaadiPaolo SpagnoloT. J. SloanE. FeiglX. HuangC. RankinPaolo LaurelliO. CallotPaolo AzzurriGünther DissertoriB. RenschDominique PallinMarco CattaneoStefan SimionG. HughesQ. OuyangT. R. EdgecockJoseph RothbergG. BolognaGerardo GanisPiero Giorgio VerdiniB. MichelG. GianniniS. NataliR. BeuselinckPhilippe GhezG. TriggianiM. C. LemaireA. M. BencheikhR. HagelbergA. BeddallH. HuI. AbtWerner WiedenmannF. ThomsonM. Bardadin-otwinowskaP. PalazziA. P. BetteridgeStephanie BrandtJ. J. VeilletAndré RougéG. B. TaylorP. TempestaI. EfthymiopoulosD. W. KimA. BöhrerW. KozaneckiF. CombleyD. R. BotterillH. WachsmuthC. MarkouG. BencivenniP. A. McnamaraY. S. GaoGy. WolfH. G. SanderG.p. MurtasP. SaraivaY. SaadiG. BonviciniR. St. DenisS. SchaelB. PietrzykB. VallageDavid CollingT. WildishF. FortiG. A. CowanH.y. KimD. J. CandlinW. OrejudosR. P. JohnsonW. BlumF. RagusaD. CasperArnaud LucotteD. Si MohandJ.r. HansenF. BossiA. PutzerM. De PalmaJ.m. YamartinoG. FeliciLorenzo FoàP. MaleyC. K. BowderyP. S. MarrocchesiC. GrupenS. GonzalezA. RanieriB. MarxE. B. MartinDonato CreanzaK. TittelKonrad KleinknechtRoger FortyF. SanchezS.r. ArmstrongD. E. JaffeR. Della MarinaJ. GrahlJohn T HarveyF. FosterGiovanna SelvaggiF. PodlyskiAlessandro GiassiP. CoyleL. PassalacquaPhilippe OdierM. WunschJ. J. AubertO. SchneiderD. BuskulicA. PachecoS. EmeryCristinel DiaconuL. SmolikChristian BauerM. ZhengM. ThulasidasKevin M. SmithGuido TonelliF. StephanI. G. KnowlesW. TejessyJ. M. RossignolA. M. GreeneGiuseppe RasoF. Le DiberderV. GaitanW. ZhaoJ. CarrB. JostL. MonetaPatrick JanotA. GallaG. GelaoM. DelfinoAlberto MessineoV. BertinG.a. BlairRoberto TenchiniC. RaineB. Bloch-devauxPablo Rodriguez PerezMaria GironeL. BosisioG. RudolphJ.a. StrongA. RoussarieS. MonteilGiuseppe ZitoG. RizzoH.j. ParkIan R TomalinC. GeorgiopoulosJ. M. ScarrAlexander FinchF. RomanoJ. SchwindlingM. LethoD. M. BinnieEttore FocardiJohn RanderIan DawsonMario GiorgiA. MintenAndrea VenturiA. BonissentA. BonissentNancy MarinelliLaurent DuflotLester D.r. ThompsonF. EtienneO.j. HayesR. SettlesJ. P. SchullerYuehong XieYang GaoJ. L. HartonK. ZachariadouM. ApollonioP. PerrodoGiuseppe BagliesiM. Fernandez-bosmanPeter ElmerA. EngelhardtFabrizio PallaI. De BonisGeorg ZobernigMi ParsonsS. OrteuI. NikolicC. GuicheneyJoleen PaterG. LutzR. WankeM. G. GreenW. CameronHasko StenzelEric LanconI. FerranteRobert RichterG. CrawfordC. VanniniD. L. JohnsonB. GobboL. BellantoniAristotelis KyriakisM. G. SmithG. ParriniH. G. MoserT. FearnleyM. H. SchuneA. FarillaI. LehrausM. DavierM. JacquetJ. F. PusztaszeriJ. K. SedgbeerH. DrevermannDuccio AbbaneoM. ChmeissaniJ. F. RenardyElizabeth LocciA. M. LutzT. MedcalfMarkus FrankJ. C. ThompsonVivek SharmaA. GregorioSau Lan WuH. MeinhardP. Van GemmerenM. CordenS. XueA. Rosado-schlosserAlan M. LitkeAndrea SciabàP. BourdonD. DecampC. GewenigerL. RolandiJie ZhangS. J. DorrisD. NicodJ. M. CrespoMario MaggiR. G. JacobsenO. BraunA. AntonelliR. TanakaA. VayakiM.g. SchmidtJoseph ProriolGiorgio MaggiA. LusianiDuncan A. BrownMossadek TalbyJ. A. PerlasE. E. KlugeF. TeubertVitaliano CiulliDavid RousseauJ. LefrançoisM. VerderiAlain FalvardF. RanjardW. MännerC. GoyEmmerich KneringerA. BarresA. MoutoussiR. BoswellF. DydakF. DydakG. BujosaLei ZhangA. KoksalB. RenkRoberto Dell'orsoVal O'sheaLl. M. MirChristian ZeitnitzI. C. ParkJørgen Beck HansenStephen HaywoodG. R. BonneaudN. KonstantinidisJorg WotschackPh. HeusseA. M. WalshM. RumpfP. GirtlerY. B. PanF. RuggieriPeter HansenE. SimopoulouV. HeppDavid CalvetLl. GarridoS. ThornG. GraefeP. ReevesL. M. BryantT. J. BrodbeckM. SchmellingP. MatoG. LuttersB.s. NilssonT. OestZ. Y. FengJ. Minguet-rodriguezF. RiveraG. San MartinMaria Agnese CiocciFabio CeruttiR. W. ClifftJ.g. LynchP. ComasLucia SilvestrisC. BozziU. BeckerA. W. HalleyJ. C. BrientTing-chi WangJane NachtmanI.j. ScottA. PascualH. SeywerdW. WitzelingW. M. NewtonJ. KnoblochAnna ColaleoD. SchlatterF. AriztizabalZiad AjaltouniJean-francois GrivazG. CalderiniJ. RaabP. J. DornanA. BlondelA. BlondelA. TrabelsiJ. SteinbergerE. FernandezW. T. MortonP. PerretG. MusolinoA. ValassiHubert KrohaG. Capon

subject

PhysicsParticle physicsMeson[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]Physics and Astronomy (miscellaneous)010308 nuclear & particles physicsElectron–positron annihilationmedia_common.quotation_subjectPhysicsHadronRest frame01 natural sciencesNuclear physicsPionExcited state0103 physical sciencesBeauty[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B mesonProduction (computer science)010306 general physicsALEPH experimentParticle Physics - Experimentmedia_common

description

A data sample of about 3.0 million hadronicZ decays collected by the ALEPH experiment at LEP in the years 1991 through 1994 is used to make an inclusive selection of B hadron events. In this event sample 4227±140±252B* mesons in the decayB*→Bγ and 1944±108±161B** u,d mesons decaying into a B meson and a charged pion are reconstructed. Here and in the followingB** u,d denotes the eightL=1(bū) and (bd) states and their charge conjugate. For the well establishedB* meson the following quantities are obtained:ΔM=M B*−MB=(45.30±0.35±0.87) MeV/c2 andN B*/(N B+N B*)=(77.1±2.6±7.0)%. The angular distribution of the photons in theB* rest frame is used to measure the relative contribution of longitudinalB* polarization states to beσ L/(σ L+σ T)=(33±6±5)%. In theM(Bπ)−M(B) mass difference resonance structure is observed at (424±4±10) MeV/c2, for which the shape and position is consistent with the expectation forB** u,d states decaying intoB(*)π ±. The relative production rate is determined to be $$\begin{gathered} \frac{{BR(Z \to b \to B_{u,d}^{ * * } )}}{{BR(Z \to b \to B_{u,d} )}} \hfill \\ = [27.9 \pm 1.6(stat) \pm 5.9(syst) {}_{ - 5.6}^{ + 3.9} (model)]\% \hfill \\ \end{gathered} $$ where the third error reflects the uncertainty due to different production and decay models for the broadB** u,d states.

10.1007/bf02907419http://hdl.handle.net/10281/390221