6533b86dfe1ef96bd12c9741

RESEARCH PRODUCT

Angular analysis of charged and neutral B → Kμ + μ − decays

L CollaborationR AaijB AdevaM AdinolfiA AffolderZ AjaltouniJ AlbrechtF AlessioM AlexanderS AliG AlkhazovPa CartelleAaa JrS AmatoS AmerioY AmhisL AnL AnderliniJ AndersonR AndreassenM AndreottiJe AndrewsRb ApplebyOa GutierrezF ArchilliA ArtamonovM ArtusoE AslanidesG AuriemmaM BaalouchS BachmannJj BackA BadalovV BalaguraW BaldiniRj BarlowC BarschelS BarsukW BarterV BatozskayaT BauerA BayJ BeddowF BedeschiI BediagaS BelogurovK BelousI BelyaevE Ben-haimG BencivenniS BensonJ BentonA BerezhnoyR BernetM-o BettlerMv BeuzekomA BienS BifaniT BirdA BizzetiPmb OrnstadT BlakeF BlancJ BlouwS BluskV BocciA BondarN BondarW BoniventoS BorghiA BorgiaM BorsatoTjv BowcockE BowenC BozziT BrambachJvd BrandJ BressieuxD BrettM BritschT BrittonNh BrookH BrownA BurscheG BusettoJ BuytaertS CadedduR CalabreseO CallotM CalviMc GomezA CamboniP CampanaDc PerezA CarboneG CarboniR CardinaleA CardiniH Carranza-mejiaL CarsonKc AkibaG CasseL CassinaLc GarciaM CattaneoC CauetR CenciM CharlesP CharpentierS-f CheungN ChiapoliniM ChrzaszczK CibaXc VidalG CiezarekPel ClarkeM ClemencicHv CliffJ ClosierC CocaV CocoJ CoganE CognerasP CollinsA Comerma-montellsA ContuA CookM CoombesS CoquereauG CortiM CorvoI CountsB CouturierGa CowanDc CraikMc TorresS CunliffeR CurrieC D'ambrosioJ DalsenoP DavidPny DavidA DavisKd BruynSd CapuaMd CianJmd MirandaLd PaulaWd SilvaPd SimoneD DecampM DeckenhoffLd BuonoN DéléageD DerkachO DeschampsF DettoriAd CantoH DijkstraS DonleavyF DordeiM DorigoAd SuárezD DossettA DovbnyaF DupertuisP DuranteR DzhelyadinA DziurdaA DzyubaS EasoU EgedeV EgorychevS EidelmanS EisenhardtU EitschbergerR EkelhofL EklundIe RifaiC ElsasserS EsenT EvansA FalabellaC FärberC FarinelliS FarryD FergusonVf AlborFf RodriguesM Ferro-luzziS FilippovM FioreM FioriniM FirlejC FitzpatrickT FiutowskiM FontanaF FontanelliR FortyO FranciscoM FrankC FreiM FrosiniJ FuE FurfaroAg TorreiraD GalliS GalloriniS GambettaM GandelmanP GandiniY GaoJ GarofoliJg TicoL GarridoC GasparR GauldL GavardiE GersabeckM GersabeckT GershonP GhezA GianelleS Giani'V GibsonL GiubegaVv GligorovC GöbelD GolubkovA GolutvinA GomesH GordonC GottiMg GándaraRg DiazLag CardosoE GraugésG GrazianiA GrecuE GreeningS GregsonP GriffithL GrilloO GrünbergB GuiE GushchinY GuzT GysC HadjivasiliouG HaefeliC HaenSc HainesS HallB HamiltonT HampsonX HanS Hansmann-menzemerN HarnewSt HarnewJ HarrisonT HartmannJ HeT HeadV HeijneK HennessyP HenrardL HenryJah MorataEv HerwijnenM HeßA HicheurD HillM HoballahC HombachW HulsbergenP HuntN HussainD HutchcroftD HyndsM IdzikP IltenR JacobssonA JaegerJ JalochaE JansP JatonA JawaheryM JezabekF JingM JohnD JohnsonCr JonesC JoramB JostN JurikM KaballoS KandybeiW KansoM KaracsonTm KarbachM KelseyIr KenyonT KetelB KhanjiC KhurewathanakulS KlaverO KochebinaM KolpinI KomarovRf KoopmanP KoppenburgM KorolevA KozlinskiyL KravchukK KreplinM KrepsG KrockerP KrokovnyF KruseM KucharczykV KudryavtsevK KurekT KvaratskheliyaVnl ThiD LacarrereG LaffertyA LaiD LambertRw LambertE LanciottiG LanfranchiC LangenbruchB LanghansT LathamC LazzeroniRl GacJv LeerdamJ-p LeesR LefèvreA LeflatJ LefrançoisS LeoO LeroyT LesiakB LeveringtonY LiM LilesR LindnerC LinnF LionettoB LiuG LiuS LohnI LongstaffJh LopesN Lopez-marchP LowdonH LuD LucchesiH LuoA LupatoE LuppiO LuptonF MachefertIv MachikhiliyanF MaciucO MaevS MaldeG MancaG MancinelliM ManzaliJ MaratasJf MarchandU MarconiCm BenitoP MarinoR MärkiJ MarksG MartellottiA MartensAm SánchezM MartinelliDm SantosFm VidalDm TostesA MassafferriR MatevZ MatheC MatteuzziA MazurovM MccannJ MccarthyA McnabR McnultyB McskellyB MeadowsF MeierM MeissnerM MerkDa MilanesM-n MinardJm RodriguezS MonteilD MoranM MorandinP MorawskiA MordàMj MorelloJ MoronR MountainF MuheimK MüllerR MuresanB MusterP NaikT NakadaR NandakumarI NastevaM NeedhamN NeriS NeubertN NeufeldM NeunerAd NguyenTd NguyenC Nguyen-mauM NicolV NiessR NietN NikitinT NikodemA NovoselovA Oblakowska-muchaV ObraztsovS OggeroS OgilvyO OkhrimenkoR OldemanG OnderwaterM OrlandeaJmo GoicocheaP OwenA OyangurenBk PalA PalanoF PalomboM PalutanJ PanmanA PapanestisM PappagalloC ParkesCj ParkinsonG PassalevaGd PatelM PatelC PatrignaniAp AlvarezA PearceA PellegrinoMp AltarelliS PerazziniEp TrigoP PerretM Perrin-terrinL PescatoreE PesenK PetridisA PetroliniEp OlloquiB PietrzykTp VrD PinciA PistoneS PlayferMp CasasusF PolciA PoluektovE PolycarpoA PopovD PopovB PopoviciC PotteratA PowellJ PrisciandaroA PritchardC ProuveV PugatchAp NavarroG PunziW QianB RachwalJh RademackerB RakotomiaramananaM RamaMs RangelI RaniukN RauschmayrG RavenS ReichertMm ReidAcd ReisS RicciardiA RichardsK RinnertVr MolinaDar RomeroP RobbeAb RodriguesE RodriguesPr PerezS RoiserV RomanovskyAr VidalM RotondoJ RouvinetT RufF RuffiniH RuizPr VallsG SabatinoJjs SilvaN SagidovaP SailB SaittaVs GuimaraesCs MayordomoBs SedesR SantacesariaCs RiosE SantovettiM SapunovA SartiC SatrianoA SattaM SavrieD SavrinaM SchillerH SchindlerM SchluppM SchmellingB SchmidtO SchneiderA SchopperM-h SchuneR SchwemmerB SciasciaA SciubbaM SecoA SemennikovK SenderowskaI SeppN SerraJ SerranoL SestiniP SeyfertM ShapkinI ShapovalY ShcheglovT ShearsL ShekhtmanV ShevchenkoA ShiresRs CoutinhoG SimiM SirendiN SkidmoreT SkwarnickiNa SmithE SmithE SmithJ SmithM SmithH SnoekMd SokoloffFjp SolerF SoomroD SouzaBsd PaulaB SpaanA SparkesF SpinellaP SpradlinF StagniS StahlO SteinkampO StenyakinS StevensonS StoicaS StoneB StoraciS StrackaM StraticiucU StraumannR StroiliVk SubbiahL SunW SutcliffeK SwientekS SwientekV SyropoulosM SzczekowskiP SzczypkaD SzilardT SzumlakS T'jampensM TeklishynG TellariniE TeodorescuF TeubertC ThomasE ThomasJv TilburgV TisserandM TobinS TolkL TomassettiD TonelliS Topp-joergensenN TorrE TournefierS TourneurMt TranM TreschA TsaregorodtsevP TsopelasN TuningMu GarciaA UklejaA UstyuzhaninU UwerV VagnoniG ValentiA VallierRv GomezPv RegueiroCv SierraS VecchiJj VelthuisM VeltriG VenezianoM VesterinenB ViaudD VieiraMv DiazX Vilasis-cardonaA VollhardtD VolyanskyyD VoongA VorobyevV VorobyevC VoßH VossJad VriesR WaldiC WallaceR WallaceJ WalshS WandernothJ WangDr WardNk WatsonAd WebberD WebsdaleM WhiteheadJ WichtD WiednerG WilkinsonMp WilliamsM WilliamsFf WilsonJ WimberleyJ WishahiW WislickiM WitekG WormserSa WottonS WrightS WuK WyllieY XieZ XingZ XuZ YangX YuanO YushchenkoM ZangoliM ZavertyaevF ZhangL ZhangWc ZhangY ZhangA ZhelezovA ZhokhovL ZhongA Zvyagin

subject

B physic12.15.MmB physicsSettore FIS/04 - Fisica Nucleare e SubnucleareLuminosityNeutral currentFlavor physicsMathematics::ProbabilityNuclear Experimentmedia_commonPhysicsB physics; Flavor physics; Flavour changing neutral currents; Hadron-hadron scattering; Rare decayPhysicsPHYSICS PARTICLES & FIELDSParticle physicsAmplitudePhysical SciencesFísica nuclearLHCNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subject14.40.NdScalar (mathematics)Flavour Changing Neutral CurrentsMathematics::Analysis of PDEsLHCb - Abteilung HofmannHadronsMeasure (mathematics)AsymmetryMathematics::Numerical AnalysisStandard ModelAngular distributionTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYLeptonic semileptonic and radiative decays of bottom mesonSDG 7 - Affordable and Clean EnergyTensorLarge Hadron Collider (France and Switzerland)Science & Technology/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyHadron-Hadron ScatteringGran Col·lisionador d'HadronsFlavour changing neutral currentLHCbRare decay13.20.HeFlavor physicBottom mesons (|B|>0)High Energy Physics::ExperimentFísica de partículesExperiments

description

The angular distributions of the rare decays B → K+µ+µ- and B0 → K0 <inf>a</inf>Sμ+μ- are studied with data corresponding to 3 fb-1 of integrated luminosity, collected in proton-proton collisions at 7 and 8TeV centre-of-mass energies with the LHCb detector. The angular distribution is described by two parameters, FH and the forward-backward asymmetry of the dimuon system AFB, which are determined in bins of the dimuon mass squared. The parameter F<inf>H</inf> is a measure of the contribution from (pseudo)scalar and tensor amplitudes to the decay width. The measurements of A<inf>FB</inf> and F<inf>H</inf> reported here are the most precise to date and are compatible with predictions from the Standard Model.

10.1007/jhep05(2014)082http://hdl.handle.net/11567/777623