6533b82bfe1ef96bd128d672
RESEARCH PRODUCT
First observation and measurement of the decay K±→π±e+e−γ
Rainer WankeR. FantechiA. CeccucciAndrea BizzetiMarco ClemencicF. CostantiniC. CerriI. PolenkevichM. D. WoodMilene CalvettiG. RuggieroG.m. PierazziniJ. DerreI. MannelliA. GonidecB. VallageE. C. SwallowP. RubinRoberta ArcidiaconoH. D. WahlM. FidecaroEvgueni GoudzovskiN. DobleH. DibonG. CollazuolS. BalevM. MartiniR. WinstonB. PeyaudL. MasettiD. CowardCristina LazzeroniJ.b. ChezeM. ScarpaT. Fonseca MartinM. HolderMauro RaggiB. RenkMauro PicciniP. HristovLuca FioriniA.j. CullingE. MarinovaE. MonnierG. NeuhoferD.j. MundayG. MarelA. WinhartNicola CabibboW. KubischtaM. ShiehC. CheshkovV. KozhuharovD.c. CundyS. StoynevNicolo CartigliaM. PepeCristina BiinoIvan MikulecLau GatignonM. SavrieE. IacopiniA. A. MaierP. F. DalpiazP. MarouelliB. Bloch-devauxP. CenciC. HandelM. VeltriF. MarchettoC. DamianiM.w. SlaterL. WidhalmManfred JeitlerW. BaldiniG.e. KalmusV. FalaleevA. ZinchenkoM. ZiolkowskiM. De BeerG. AnzivinoJ. R. BatleyA. PetersS. Goy LopezA. NortonM. BehlerG. BocquetYu. PotrebenikovA. NappiS. WottonVladimir KekelidzeS. GiudiciM. SozziL. DilellaM. WacheMassimiliano FioriniD. T. MadigozhinE. MazzucatoC. Morales MoralesMayda VelascoM. MarkytanM. LentiA. GianoliEnrico CeleghiniA. DabrowskiM. C. PetrucciMaulik R. PatelKonrad KleinknechtM. Valdata-nappiF. MartelliM. SzleperSimone BifaniU. MoosbruggerE. ImbergamoA. Cotta RamusinoG. LamannaFabrizio PetrucciLeander LitovAlan W. WalkerP. L. FrabettiA. MichettiN. A. MolokanovaK. Eppardsubject
PhysicsNuclear and High Energy PhysicsAntiparticleChiral perturbation theoryMeson010308 nuclear & particles physicsBranching fractionHadronAnalytical chemistry01 natural sciencesNuclear physicsParticle decayPion0103 physical sciences010306 general physicsDimensionless quantitydescription
Abstract Using the full data set of the NA48/2 experiment, the decay K ± → π ± e + e − γ is observed for the first time, selecting 120 candidates with 7.3 ± 1.7 estimated background events. With K ± → π ± π D 0 as normalisation channel, the branching ratio is determined in a model-independent way to be Br ( K ± → π ± e + e − γ , m e e γ > 260 MeV / c 2 ) = ( 1.19 ± 0.12 stat ± 0.04 syst ) × 10 −8 . This measured value and the spectrum of the e + e − γ invariant mass allow a comparison with predictions of chiral perturbation theory.
year | journal | country | edition | language |
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2008-01-01 | Physics Letters B |