6533b873fe1ef96bd12d562a

RESEARCH PRODUCT

Observation of the Decay D0→K−π+e+e−

C. BüngerStephen SekulaA. OyangurenA. JawaheryC. BozziJ. ChauveauF. De MoriK. HonscheidE. A. KozyrevE. A. KozyrevN. TasneemHeiko LackerAidan Randle-condeR. J. BarlowG. R. BonneaudR. CenciC. TouramanisA. ZalloFlorian Urs BernlochnerG. CibinettoB. BhuyanF. PalomboT. LueckB. G. FulsomE. P. SolodovE. P. SolodovT. S. MiyashitaS. BettariniS. PrellO. GrünbergD. W. G. S. LeithMaurizio BiasiniM. PosoccoG. CalderiniJames H CochranJ. L. RitchieI. M. PeruzziR. GorodeiskyD. A. RobertsS. I. SerednyakovS. I. SerednyakovA. G. DenigK. R. SchubertOwen Rosser LongH. A. NealG. CasarosaA. M. RossiF. BianchiA. LusianiV. P. DruzhininV. P. DruzhininV. PoireauT. S. MattisonV. B. GolubevV. B. GolubevG. WormserJ. A. ErnstW. GradlA. PalanoT. SchroederA. HafnerJoseph IzenL. LanceriS. EmeryR. Y. SoM. BellisS. DittrichC. HeartyP. OngmongkolkulC. HastD. J. LangeG. PireddaW. J. WisniewskiE. M. T. PuccioA. R. BuzykaevM. S. AlamM. T. GrahamEleonora LuppiM. PiccoloA. P. OnuchinA. P. OnuchinA. P. OnuchinA. BeaulieuS. MartellottiM. CarpinelliL. M. CremaldiJ. M. RoneyL. SunT. J. GershonB. EchenardJames R. WilsonG. BatignaniZ. C. HuardW. Panduro VazquezG. J. KingS. LuitzD. BernardP. C. KimM. V. PurohitD. J. SummersP. PatteriD. G. HitlinW. R. InnesR. F. SchwittersJ. Va’vraE. A. KravchenkoE. A. KravchenkoJ. AlbertA. FilippiElisa ManoniColin JessopR. PrepostD. AstonJ. G. SmithR. C. FieldE. Ben-haimAdrian John BevanF. FortiW. S. LockmanCrisostomo SciaccaF. AnulliW. DunwoodieR. CowanJ. DorfanJ. J. WalshY. LiA. M. EisnerI. M. NugentAlessandro GazA. CalcaterraI> Ar<B. G. PushpawelaTim AdyeR. SaccoD. N. BrownA. M. LutzR. D. KassM. BombenR. J. SobieG. FinocchiaroSw. BanerjeeC. H. ChengT. E. LathamS. H. RobertsonL. VitaleF. Di LodovicoG. EigenR. De SangroS. PassaggioS. L. WuR. FacciniF. FerrarottoA. J. LankfordF. Martinez-vidalC. CartaroDominik MüllerJ. P. LeesD. J. PayneHerbert KochF. Le DiberderG. D. LaffertyN. ArnaudR. KowalewskiM. RotondoF. F. WilsonM. R. ConveryA. J.s. SmithYu. I. SkovpenYu. I. SkovpenG. De NardoAbner SofferD. S. ChaoB. OberhofM. RöhrkenSimon AkarYu G. KolomenskyK. GriessingerK. Yu. TodyshevK. Yu. TodyshevB. N. RatcliffM. DavierV. SantoroB. T. MeadowsG. VasseurA. RoodmanG. A. CowanDouglas WrightK. T. FloodG. RavenR. GodangR. M. SeddonM. D. SokoloffE. FioravantiL. ZaniP. R. BurchatE. PaoloniR. StroiliRoland WaldiP. TarasAlessandro PilloniF. FerroniD. R. PeimerRoberto CalabreseD. B. MacfarlaneD. GambaM. RamaPaul Fraser HarrisonJ. A. MckennaJu-young KimStephen Robert WagnerHamad AhmedJ. OcarizM. K. SullivanN. GuttmanM. HeßJ. W. GaryJ. P. ColemanE. GraugesMario GiorgiR. CheaibG. MarchioriE. GabathulerF. C. PorterSpan> B<F. SimonettoJ. M. LoseccoB. DeyC. H. ChenX. C. LouS. M. SpanierMartino MargoniM. ChrzaszczC. VoßVladimir BlinovVladimir BlinovVladimir BlinovD. BettoniAndrei GritsanI. GarziaD. E. HutchcroftC. PatrignaniG. RizzoV. TisserandT. LeddigM. VerderiU. MallikN. NeriM. FritschGabriele SimiC. L. DavisM. Ebert

subject

PhysicsParticle physicsAnnihilationBranching fraction0103 physical sciencesGeneral Physics and AstronomyResonanceInvariant mass010306 general physics01 natural sciencesEnergy (signal processing)Standard Model

description

We report the observation of the rare charm decay D^{0}→K^{-}π^{+}e^{+}e^{-}, based on 468  fb^{-1} of e^{+}e^{-} annihilation data collected at or close to the center-of-mass energy of the ϒ(4S) resonance with the BABAR detector at the SLAC National Accelerator Laboratory. We find the branching fraction in the invariant mass range 0.675<m(e^{+}e^{-})<0.875  GeV/c^{2} of the electron-positron pair to be B(D^{0}→K^{-}π^{+}e^{+}e^{-})=(4.0±0.5±0.2±0.1)×10^{-6}, where the first uncertainty is statistical, the second systematic, and the third due to the uncertainty in the branching fraction of the decay D^{0}→K^{-}π^{+}π^{+}π^{-} used as a normalization mode. The significance of the observation corresponds to 9.7 standard deviations including systematic uncertainties. This result is consistent with the recently reported D^{0}→K^{-}π^{+}μ^{+}μ^{-} branching fraction, measured in the same invariant mass range, and with the value expected in the standard model. In a set of regions of m(e^{+}e^{-}), where long-distance effects are potentially small, we determine a 90% confidence level upper limit on the branching fraction B(D^{0}→K^{-}π^{+}e^{+}e^{-})<3.1×10^{-6}.

https://doi.org/10.1103/physrevlett.122.081802