6533b7cefe1ef96bd12579c2
RESEARCH PRODUCT
E decays to ηππ in annihilation at rest
R. BossinghamN. DjaoshviliK. BeuchertJ. BroseN. WinterP. BlümD. JamnikN.p. HesseyD. EngelhardtS. SpanierC. KoloR. HackmannM. A. FaesslerD.v. BuggR. OuaredR.p. HaddockR. LanduaI. ScottP. SchmidtČ. ZupančičF. H. HeinsiusP. GiarrittaPàl HidasC. VölckerO. CramerJ. KisielW. DünnweberR. MccradyC. A. MeyerU. WiednerP. BirienMichael DoserC. HolzhaußenM. SchütrumpfB.s. ZouE. SchäferF. Ould-saadaMarcel KunzeK. BrauneC. RegenfusH. KalinowskyK. PetersT. CaseH. MatthäyH. StöckB. KalteyerC.a. BakerClaude AmslerM. EnglertA. CooperM. TischhäuserF. WalterT. DegenerA. NobleJ. ZollM. HerzM. BenayounU. ThomaKenneth M. CroweD. UrnerHerbert KochG. PinterB. M. BarnettD. WaltherJ. P. MerloU. StrohbuschC. StraßburgerL. MontanetJ. LüdemannC.j. BattyS. RavndalEberhard KlemptT. KielH. P. DietzC. N. PinderS. V. DombrowskiD. S. ArmstrongM. LakataB. KämmleP. IllingerM. SuffertR. Seibertsubject
Nuclear physicsPhysicsNuclear and High Energy PhysicsAngular distributionAnnihilationMesonBranching fractionIsoscalarMass spectrumdescription
Abstract We have observed the ηπ + π − and ηπ 0 π 0 decay modes of the E meson in p p annihilation at rest into π + π − π 0 π 0 η . The mass and width of the E meson are 1409 ± 3 and 86 ± 10 MeV. The production and decay branching ratio is B( p p → Eππ)B(E → ηππ) = (3.3 ± 1.0) × 10 −3 . With a spin-parity analysis we determine that J P = 0 − . The observation of the ηπ 0 π 0 decay mode establishes that E is isoscalar ( C = +1). We find that E decays to η ( ππ ) s (where ( ππ ) s is an S-wave dipion) and πa 0 (980)(→ πη ) with a relative branching ratio of (78 ± 16) %. Using the K K π production and decay branching ratio measured earlier we determine that B[E → K K π] B[E → ηππ] = 0.61 ± 0.19 . A comparison with observations in radiative J Ψ decays suggests that E and ι η (1416) are identical.
year | journal | country | edition | language |
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1995-09-01 | Physics Letters B |