6533b825fe1ef96bd128278c
RESEARCH PRODUCT
A test of chiral perturbation theory from the measurement of the decay KS → γγ
H. G. SanderA. NappiM. CalvettiM. RostP. GrafströmO. PerdereauArthur SchafferD.c. CundyD. CowardJ. ScheidtA. KreutzM. PunturoPaolo CalafiuraV.m. MarzulliA. WagnerI. MannelliC. CerriT. BeierR. HagelbergF. LeberM. HolderG.m. PierazziniR. CarosiH. D. WahlLydia Iconomidou-fayardR. CasaliPeter BuchholzL. GatignonB. RenkG.d. BarrL. BertanzaF. ScheererN. DobleKonrad KleinknechtKen PeachDaniel FournierE. AugéH. BlümerR. WerthenbachLaurent SerinJ. Staecksubject
PhysicsNuclear physicsSystematic errorNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryBranching fractiondescription
Data from NA31 experiment at CERN have been used to measure the decay KS → γγ. From 69 candidate events of the type K0 → γγ, 52 events can be attributed to KL → γγ and one event is expected from background processes. The ratio of the relative decay widths R = Γ(KS → γγ)Γ(KL → γγ) is measured to be R = 2.2 ± 1.0(stat.) ± 0.3(syst.) ± 0.2(ext.) where the external systematic error is due to the experimental uncertainty in the branching ratio of the decay KL → γγ. This translates into a branching ratio of BR(KS → γγ) = (2.2 ± 1.1) × 10−6. If these data are combined with the published data from an earlier data taking period with the same experiment, the ratio R is determined to be R = 2.35 ± 0.75(stat.) ± 0.4(syst.) + 7.5 · (1 − BR(KL → γγ)5.86 × 10−4) where the last term accounts for the dependence on the measured KL → γγ branching ratio. The corresponding branching ratio for KS → γγ is BR(KS → γγ) = (2.4 ± 0.9) × 10−6. The measurement is a sensitive test of chiral perturbation theory and in good agreement with theoretical predictions.
year | journal | country | edition | language |
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1995-06-01 | Physics Letters B |