6533b7d6fe1ef96bd1266ea4
RESEARCH PRODUCT
Measurement of the resonant andCPcomponents inB¯0→J/ψπ+π−decays
W. SutcliffeL. BeaucourtP. DuranteA. PetroliniG. BusettoS. GambettaMax NeunerV. NiessSilvia BorghiN. HussainP. LowdonM. KaracsonE. GraugesE. GreeningI. LongstaffA. Romero VidalA. B. RodriguesO. MaevTomasz SkwarnickiSebastian BachmannF. TeubertJ. LefrançoisF. Martinez VidalG. ValentiC. LangenbruchN. NeriS. T. HarnewF. MachefertC. HombachN. TuningTjeerd KetelM. RotondoMartino BorsatoW. C. ZhangN. RauschmayrN. A. SmithE. Van HerwijnenR. EkelhofP. OwenH. LuV. ObraztsovStephan EisenhardtM. RamaF. FontanelliW. BaldiniJ. BlouwMatthew KelseyR. CurriePatrick KoppenburgLei ZhangA. GianelleD. R. JohnsonA. PowellB. RakotomiaramananaC. R. JonesE. Ben-haimJ. AlbrechtA. SemennikovD. BrettS. Hansmann-menzemerA. SchopperM. HeßC. ParkesXiaoxue HanF. RuffiniM. KorolevI. El RifaiF. KruseR. SchwemmerN. ChiapoliniR. MountainYang LiM. SavrieV. HeijneJ. Garra TicoT. HeadI. SeppX. YuanMarianna FontanaR. AndreassenF. MaciucSandro CadedduS. AmerioW. WislickiS. EasoB. SchmidtB. Sanmartin SedesYejin ZhangR. NandakumarMiroslaw FirlejPatrick RobbeJ. GarofoliJonas RademackerF. MuheimM. VeltriG. HaefeliG. AlkhazovC. ProuveT. LesiakV. GibsonA. SattaC. KhurewathanakulC. Santamarina RiosS. StoicaPietro MarinoS. GregsonLaura GavardiA. BorgiaUlrik EgedeJ. A. De VriesT. RufDmitry GolubkovR. LindnerStephen M. StahlStephane T'jampensA. MartensXavier Vilasis-cardonaBarbara SciasciaS.i. EidelmanMichael KolpinG. WormserF. ZhangG. MartellottiE. LanciottiA. ShiresS. LohnS. PerazziniAlexander BerezhnoyJ. P. LeesH. L. SnoekE. S. SmithN. NeufeldG. LanfranchiM.-n. MinardA. D. NguyenJ. R. SmithValery PugatchJ. BentonA. VorobyevMarek JezabekF. DordeiJ. MccarthyTara ShearsR. WallaceWilliam BarterP. SailR. SantacesariaA. VallierDenis DerkachAngelo CarboneJaap VelthuisF. J. P. SolerX. Cid VidalC. SatrianoS. AliT. M. KarbachI. NastevaA. NovoselovN. MoggiAnton PoluektovLorenzo SestiniA. CookM. Calvo GomezN. TorrGuoming LiuW. D. HulsbergenMariana RihlS. OggeroS. LeoKonstantinos PetridisI. ShapovalA. ContuF. Ferreira RodriguesD. FergusonA. RichardsAgnieszka Oblakowska-muchaA. ZhelezovB. Souza De PaulaM. FioreMarco AdinolfiA. DavisG. WilkinsonG. MancaO. SchneiderA. Pazos AlvarezM. SapunovG. VenezianoR. Vazquez GomezMark WhiteheadM. Vieites DiazG. CortiD. SouzaS. FilippovOlivier LeroyW. KansoW. De SilvaR. NietA. ZvyaginP. SzczypkaM. P. WilliamsS. MaldeLucio AnderliniLucio AnderliniOscar De Aguiar FranciscoM. PatelL. PescatoreS. C. HainesA. HicheurE. FurfaroR. MuresanN. K. WatsonA. KozlinskiyD. TonelliJ. WimberleyA. DovbnyaB. LanghansBo LiuV. BocciD. LacarrereA. MordàG. PunziF. SoomroV. VorobyevD. Martins TostesO. YushchenkoM. MccannS. NeubertV. ShevchenkoC. MatteuzziM. CoombesG. TellariniMarkus FrankA. VollhardtMichael AlexanderKarol HennessyM. Ferro-luzziJ. J. WalshG. D. PatelS. PlayferS. WrightHoward GordonD. MoranA. SparkesM. KaballoIvan BelyaevA. PopovH. LuoMassimiliano FioriniA. ArtamonovA. BienAlessio SartiA. A. AlvesA. A. AlvesM. CharlesC. LazzeroniM. MeissnerJ. WishahiJulien CoganB. PopoviciN. DéléageIgnacio BediagaC. Vázquez SierraA. McnabA. PapanestisS. BensonB. HamiltonC. ThomasV. Salustino GuimaraesH. BrownF. MeierV. EgorychevRoland BernetRoger BarlowS. WuT. HartmannA. GrecuL. SunR. MatevE. Picatoste OlloquiK. Carvalho AkibaMirco AndreottiD. LambertS. WandernothR. CalabreseBernardo AdevaE. ThomasP. JatonE. GersabeckG. MancinelliC. FärberJ. Van TilburgT. BrittonS. GalloriniD. HillMaurizio MartinelliM. SzczekowskiB. RachwalT. BrambachI. KomarovRobert ApplebyD. SzilardJ. F. J. Van Den BrandGiovanni CarboniU. StraumannR. DzhelyadinA. LaiA. PearceL. GarridoS. TourneurOlivier DeschampsMarco DorigoPhilip IltenG. D. LaffertyJinlin FuM. Perrin-terrinO. SteinkampFlavio ArchilliAnna LupatoM. BritschV. Fernandez AlborI. V. MachikhiliyanK. KreplinJ. MaratasM. M. ReidSimone BifaniM. TobinA. DzyubaT. HampsonKrzysztof SwientekR. MärkiFranco BedeschiTh. BauerL. KravchukAlessandro CardiniJ. M. De MirandaM. LilesD. WebsdaleB. CouturierN. SkidmoreR. CenciM. CorvoS. MonteilI. 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TolkKurt RinnertCh. ElsasserSandra AmatoH. Carranza-mejiaO. LuptonK. BelousM. SecoM. T. TranM. HoballahW. QianLouis HenryG. CiezarekA. Martín SánchezR. JacobssonF. BlancR. LefèvreK. MüllerI. CountsE. PesenNathan JurikP. HuntK. WyllieB. PietrzykD. LucchesiM. MerkL. GrilloMarta CalviSimone StrackaRoger FortyJ. WichtP. E. L. ClarkeDavid HutchcroftTomasz FiutowskiS. RicciardiC. J. ParkinsonS. VecchiR. GauldE. SantovettiP. CollinsNicola SerraG. GrazianiP. N. Y. DavidChristoph FreiAlbert BurscheJ. BressieuxMatteo ManzaliS. RoiserG. SabatinoS. KandybeiF. PalomboS. EsenU. MarconiK. KurekA. C. Dos ReisYang GaoElie AslanidesYasmine AmhisLars EklundM. ZangoliP. Vazquez RegueiroR. Silva CoutinhoDmitry PopovG. AuriemmaG. AuriemmaA. DziurdaR. Graciani DiazM. MorandinT. NikodemF. StagniNeville HarnewVladislav BalaguraZiad AjaltouniB. StoraciA.e. BondarA. OyangurenM. SmithA. JawaheryD. HyndsD. GalliM. H. SchuneD. C. CraikP. M. BjørnstadT. PilařMarco CattaneoMarina ArtusoU. UwerR. StroiliJan BuytaertF. SpinellaTimothy GershonY. XieO. KochebinaP. SpradlinS. StevensonThomas BlakeH. SchindlerMarek IdzikP. Ruiz VallsM. Plo CasasusP. SeyfertT. D. NguyenS.-f. CheungM. De CianM. Van BeuzekomScott ElyO. GrünbergJ. PrisciandaroL. TomassettiB. ViaudA. UklejaB. KhanjiN. SagidovaL. CassinaAntonio PellegrinoS. CoquereauE. PolycarpoTatsuya NakadaA. PritchardG. BencivenniB. MusterA. JaegerF. F. JingU. EitschbergerP. MorawskiW. BoniventoL. ZhongH. VossA. UstyuzhaninJ. M. Otalora GoicocheaB. McskellyC. GasparP. NaikJing WangA. MazurovS. ReichertT. BirdM. SchmellingM. NicolI. R. KenyonM. PappagalloD. PinciM. VesterinenMichal KrepsS. GianìB. JostV. RomanovskyS. DonleavyZ. XingYu. GuzMarco ClemencicP. De SimoneCarmelo D'ambrosioJean François MarchandV. Rives MolinaA. A. AffolderJ. AndersonOleg StenyakinC. FitzpatrickR. F. KoopmanC. HaenB. SpaanL. Del BuonoJ. ClosierA. MassafferriC. HadjivasiliouJ. A. Hernando MorataM. BaalouchFrancesco DettoriA. FalabellaBiagio SaittaC. WallaceJ. BeddowRoel AaijG. SimiJ. H. LopesGerco OnderwaterC. GöbelJ. E. AndrewsHans DijkstraS. BluskAlessandro CamboniZishuo YangM. PalutanE. Perez TrigoZ. MatheVarvara BatozskayaG. KrockerD. VieiraM. TeklishynM. O. BettlerL. ShekhtmanA. Dosil SuárezChung Nguyen-mauM. MussiniK. De BruynJ. HarrisonF. PolciD. A. MilanesS. Topp-joergensenV. V. GligorovM. KucharczykJeremy DalsenoM. DeckenhoffS. KlaverJ. J. Saborido SilvaThierry GysZhirui XuM. Ubeda GarciaP. Rodriguez PerezVictor CocoP. GriffithAlbert Comerma-montellsA. Puig NavarroTimothy EvansD. Campora PerezD. A. Roa RomeroV. KudryavtsevAndrea BizzetiD. R. WardS. OgilvyB. GuiM. SirendiS. SwientekP. TsopelasThomas LathamC. PatrignaniS. CunliffeV. TisserandF. F. WilsonGianluigi CasseA. GomesL. A. Granado CardosoN. H. BrookE. JansM. S. RangelLiupan AnK. CibaS. FarryM. J. MorelloP. PerretJ. HeA. PistoneO. Aquines GutierrezSergey BarsukC. JoramH. RuizE. RodriguesM. OrlandeaL. De PaulaFederica LionettoD. WiednerB. LeveringtonM. ChrzaszczL. GiubegaC. VoßL. Castillo GarciaNikolay BondarO. OkhrimenkoPh. GhezA. SciubbaJ. MarksM. StraticiucG. A. CowanD. VoongR. Le GacNathanael FarleyM. WitekM. NeedhamMalcolm JohnM. GandelmanM. TreschE. GushchinC. LinnJohn BackG. PassalevaPh. Charpentiersubject
QuarkPhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsParity (physics)01 natural sciencesOmegaSpectral lineNuclear physics0103 physical sciencesPiHigh Energy Physics::ExperimentTetraquarkInvariant mass010306 general physicsdescription
The resonant structure of the reaction (B) over bar (0) --> J/psi pi(+)pi(-) is studied using data from 3 fb(-1) of integrated luminosity collected by the LHCb experiment, one third at 7 TeV center-of-mass energy and the remainder at 8 TeV. The invariant mass of the pi(+)pi(-) pair and three decay angular distributions are used to determine the fractions of the resonant and nonresonant components. Six interfering pi(+)pi(-) states, rho(770), f(0)(500), f(2)(1270), rho(1450), omega(782) and rho(1700), are required to give a good description of invariant mass spectra and decay angular distributions. The positive and negative charge parity fractions of each of the resonant final states are determined. The f(0)(980) meson is not seen and the upper limit on its presence, compared with the observed f(0)(500) rate, is inconsistent with a model where these scalar mesons are formed from two quarks and two antiquarks (tetraquarks) at the eight standard deviation level. In the q (q) over bar model, the absolute value of the mixing angle between the f(0)(980) and the f(0)(500) scalar mesons is limited to be less than 17 degrees at 90% confidence level.
year | journal | country | edition | language |
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2014-07-10 | Physical Review D |