6533b826fe1ef96bd1284edf

RESEARCH PRODUCT

Measurement ofCPobservables inB±→DCPK±decays and constraints on the CKM angleγ

P. Del Amo SanchezJ. P. LeesV. PoireauE. PrencipeV. TisserandJ. Garra TicoE. GraugesM. MartinelliA. PalanoM. PappagalloG. EigenB. StuguL. SunM. BattagliaD. N. BrownB. HoobermanL. T. KerthYu. G. KolomenskyG. LynchI. L. OsipenkovT. TanabeC. M. HawkesA. T. WatsonH. KochT. SchroederD. J. AsgeirssonC. HeartyT. S. MattisonJ. A. MckennaA. KhanA. Randle-condeV. E. BlinovA. R. BuzykaevV. P. DruzhininV. B. GolubevA. P. OnuchinS. I. SerednyakovYu. I. SkovpenE. P. SolodovK. Yu. TodyshevA. N. YushkovM. BondioliS. CurryD. KirkbyA. J. LankfordM. MandelkernE. C. MartinD. P. StokerH. AtmacanJ. W. GaryF. LiuO. LongG. M. VitugC. CampagnariT. M. HongD. KovalskyiJ. D. RichmanA. M. EisnerC. A. HeuschJ. KrosebergW. S. LockmanA. J. MartinezT. SchalkB. A. SchummA. SeidenL. O. WinstromC. H. ChengD. A. DollB. EchenardD. G. HitlinP. OngmongkolkulF. C. PorterA. Y. RakitinR. AndreassenM. S. DubrovinG. MancinelliB. T. MeadowsM. D. SokoloffP. C. BloomW. T. FordA. GazM. NagelU. NauenbergJ. G. SmithS. R. WagnerR. AyadW. H. TokiH. JasperT. M. KarbachJ. MerkelA. PetzoldB. SpaanK. WackerM. J. KobelK. R. SchubertR. SchwierzD. BernardM. VerderiP. J. ClarkS. PlayferJ. E. WatsonM. AndreottiD. BettoniC. BozziR. CalabreseA. CecchiG. CibinettoE. FioravantiP. FranchiniE. LuppiM. MuneratoM. NegriniA. PetrellaL. PiemonteseR. Baldini-ferroliA. CalcaterraR. De SangroG. FinocchiaroM. NicolaciS. PacettiP. PatteriI. M. PeruzziM. PiccoloM. RamaA. ZalloR. ContriE. GuidoM. Lo VetereM. R. MongeS. PassaggioC. PatrignaniE. RobuttiS. TosiB. BhuyanV. PrasadC. L. LeeM. MoriiA. AdametzJ. MarksS. SchenkU. UwerF. U. BernlochnerM. EbertH. M. LackerT. LueckA. VolkP. D. DaunceyM. TibbettsP. K. BeheraU. MallikC. ChenJ. CochranH. B. CrawleyL. DongW. T. MeyerS. PrellE. I. RosenbergA. E. RubinY. Y. GaoA. V. GritsanZ. J. GuoN. ArnaudM. DavierD. DerkachJ. Firmino Da CostaG. GrosdidierF. Le DiberderA. M. LutzB. MalaescuA. PerezP. RoudeauM. H. SchuneJ. SerranoV. SordiniA. StocchiL. WangG. WormserD. J. LangeD. M. WrightI. BinghamC. A. ChavezJ. P. ColemanJ. R. FryE. GabathulerR. GametD. E. HutchcroftD. J. PayneC. TouramanisA. J. BevanF. Di LodovicoR. SaccoM. SigamaniG. CowanS. ParamesvaranA. C. WrenD. N. BrownC. L. DavisA. G. DenigM. FritschW. GradlA. HafnerK. E. AlwynD. BaileyR. J. BarlowG. JacksonG. D. LaffertyT. J. WestJ. AndersonR. CenciA. JawaheryD. A. RobertsG. SimiJ. M. TuggleC. DallapiccolaE. SalvatiR. CowanD. DujmicP. H. FisherG. SciollaM. ZhaoD. LindemannP. M. PatelS. H. RobertsonM. SchramP. BiassoniA. LazzaroV. LombardoF. PalomboS. StrackaL. CremaldiR. GodangR. KroegerP. SonnekD. J. SummersX. NguyenM. SimardP. TarasG. De NardoD. MonorchioG. OnoratoC. SciaccaG. RavenH. L. SnoekC. P. JessopK. J. KnoepfelJ. M. LoseccoW. F. WangL. A. CorwinK. HonscheidR. KassJ. P. MorrisA. M. RahimiN. L. BlountJ. BrauR. FreyO. IgonkinaJ. A. KolbR. RahmatN. B. SinevD. StromJ. StrubeE. TorrenceG. CastelliE. FeltresiN. GagliardiM. MargoniM. MorandinM. PosoccoM. RotondoF. SimonettoR. StroiliE. Ben-haimG. R. BonneaudH. BriandG. CalderiniJ. ChauveauO. HamonPh. LerusteG. MarchioriJ. OcarizJ. PrendkiS. SittM. BiasiniE. ManoniA. RossiC. AngeliniG. BatignaniS. BettariniM. CarpinelliG. CasarosaA. CervelliF. FortiM. A. GiorgiA. LusianiN. NeriE. PaoloniG. RizzoJ. J. WalshD. Lopes PegnaC. LuJ. OlsenA. J. S. SmithA. V. TelnovF. AnulliE. BaracchiniG. CavotoR. FacciniF. FerrarottoF. FerroniM. GasperoL. Li GioiM. A. MazzoniG. PireddaF. RengaT. HartmannT. LeddigH. SchröderR. WaldiT. AdyeB. FranekE. O. OlaiyaF. F. WilsonS. EmeryG. Hamel De MonchenaultG. VasseurCh. YècheM. ZitoM. T. AllenD. AstonD. J. BardR. BartoldusJ. F. BenitezC. CartaroM. R. ConveryJ. DorfanG. P. Dubois-felsmannW. DunwoodieR. C. FieldM. Franco SevillaB. G. FulsomA. M. GabareenM. T. GrahamP. GrenierC. HastW. R. InnesM. H. KelseyH. KimP. KimM. L. KocianD. W. G. S. LeithS. LiB. LindquistS. LuitzV. LuthH. L. LynchD. B. MacfarlaneH. MarsiskeD. R. MullerH. NealS. NelsonC. P. O’gradyI. OfteM. PerlT. PulliamB. N. RatcliffA. RoodmanA. A. SalnikovV. SantoroR. H. SchindlerJ. SchwieningA. SnyderD. SuM. K. SullivanS. SunK. SuzukiJ. M. ThompsonJ. Va’vraA. P. WagnerM. WeaverC. A. WestW. J. WisniewskiM. WittgenD. H. WrightH. W. WulsinA. K. YarrituC. C. YoungV. ZieglerX. R. ChenW. ParkM. V. PurohitR. M. WhiteJ. R. WilsonS. J. SekulaM. BellisP. R. BurchatA. J. EdwardsT. S. MiyashitaS. AhmedM. S. AlamJ. A. ErnstB. PanM. A. SaeedS. B. ZainN. GuttmanA. SofferP. LundS. M. SpanierR. EckmannJ. L. RitchieA. M. RulandC. J. SchillingR. F. SchwittersB. C. WrayJ. M. IzenX. C. LouF. BianchiD. GambaM. PelliccioniM. BombenL. LanceriL. VitaleN. Lopez-marchF. Martinez-vidalD. A. MilanesA. OyangurenJ. AlbertSw. BanerjeeH. H. F. ChoiK. HamanoG. J. KingR. KowalewskiM. J. LewczukI. M. NugentJ. M. RoneyR. J. SobieT. J. GershonP. F. HarrisonT. E. LathamE. M. T. PuccioH. R. BandS. DasuK. T. FloodY. PanR. PrepostC. O. VuosaloS. L. Wu

subject

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarityMeson010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrix01 natural sciencesB-factoryNuclear physicsParticle decay0103 physical sciencesD mesonCP violationB meson010306 general physics

description

Using the entire sample of 467×10^6 Υ(4S)→BB[overbar] decays collected with the BABAR detector at the PEP-II asymmetric-energy B factory at the SLAC National Accelerator Laboratory, we perform an analysis of B^± → DK^± decays, using decay modes in which the neutral D meson decays to either CP-eigenstates or non-CP-eigenstates. We measure the partial decay rate charge asymmetries for CP-even and CP-odd D final states to be A_(CP+) = 0.25±0.06±0.02 and A_(CP-) = -0.09±0.07±0.02, respectively, where the first error is the statistical and the second is the systematic uncertainty. The parameter A_(CP+) is different from zero with a significance of 3.6 standard deviations, constituting evidence for direct CP violation. We also measure the ratios of the charged-averaged B partial decay rates in CP and non-CP decays, R_(CP+) = 1.18±0.09±0.05 and R_(CP-) = 1.07±0.08±0.04. We infer frequentist confidence intervals for the angle γ of the unitarity triangle, for the strong phase difference δ_B, and for the amplitude ratio r_B, which are related to the B^- → DK^- decay amplitude by r_(B)e^(i(δB-γ)) = A(B^- → D[overbar]^(0)K^-)/A(B^- → D^(0)K^-). Including statistical and systematic uncertainties, we obtain 0.24 < r_B < 0.45 (0.06 < r_B <0.51) and, modulo 180°, 11.3° < γ < 22.7° or 80.8° < γ <99.2° or 157.3° <γ < 168.7° (7.0°<γ<173.0°) at the 68% (95%) confidence level.

https://doi.org/10.1103/physrevd.82.072004