6533b862fe1ef96bd12c76f9
RESEARCH PRODUCT
Antiproton-proton annihilation at rest into two-body final states
Claude AmslerD S ArmstrongI AugustinC A BakerB M BarnettC J BattyK BeuchertP BirienJ A BistirlichH P BlümR R BossinghamH BossyK BrauneJ BroseD V BuggM BurchellT CaseS U ChungA CooperK M CroweH P DietzS Von DombrowskiMichael DoserW DünnweberD EngelhardtM EnglertM A FaesslerC W FelixG FolgerR HackmannR P HaddockF H HeinsiusN P HesseyP HidasP IllingerD JamnikZ JávorfiH KalinowskyB KämmleT KielJ KisielE KlemptM KobelH KochC KoloK C KönigsmannM KunzeRolf LanduaJ LüdemannH MatthäyM MerkelJ P MerloC A MeyerU Meyer-berkhoutLucien MontanetA NobleF Ould-saadaK PetersG PintérS RavndalJ SalkA H SanjariE SchäferB SchmidP SchmidtS M SpanierC StrassburgerU StrohbuschMartin SuffertD UrnerC VölckerF WalterD WaltherU WiednerN WinterJulius ZollCrtomir Zupancicsubject
PhysicsParticle physicsAnnihilationPhysics and Astronomy (miscellaneous)Meson010308 nuclear & particles physicsAnalytical chemistry01 natural sciencesOmega[PHYS.ASTR.CO]Physics [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO][PHYS.ASTR.CO] Physics [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO]Antiproton0103 physical sciences010306 general physicsEngineering (miscellaneous)Particle Physics - Experimentdescription
We report measurements of branching ratios for production of a series of two meson final states in $$\bar p$$ p annihilations at rest in liquid hydrogen. We find: $$\begin{gathered} BR(\bar pp \to \pi ^ + \pi ^ - ) = (3.07 \pm 0.13) \cdot 10^{ - 3} \hfill \\ BR(\bar pp \to K^ + K^ - ) = (0.99 \pm 0.05) \cdot 10^{ - 3} \hfill \\ BR(\bar pp \to \pi ^0 \pi ^0 ) = (6.93 \pm 0.43) \cdot 10^{ - 4} \hfill \\ BR(\bar pp \to \pi ^0 \eta ) = (2.12 \pm 0.12) \cdot 10^{ - 4} \hfill \\ BR(\bar pp \to \pi ^0 \omega ) = (5.73 \pm 0.47) \cdot 10^{ - 3} \hfill \\ BR(\bar pp \to \pi ^0 \eta ') = (1.23 \pm 0.13) \cdot 10^{ - 4} \hfill \\ BR(\bar pp \to \eta \eta ) = (1.64 \pm 0.10) \cdot 10^{ - 4} \hfill \\ BR(\bar pp \to \eta \omega ) = (1.51 \pm 0.12) \cdot 10^{ - 2} \hfill \\ BR(\bar pp \to \eta \eta ') = (2.16 \pm 0.25) \cdot 10^{ - 4} \hfill \\ BR(\bar pp \to \omega \omega ) = (3.32 \pm 0.34) \cdot 10^{ - 2} \hfill \\ BR(\bar pp \to \omega \eta ') = (0.78 \pm 0.08) \cdot 10^{ - 2} \hfill \\ \end{gathered}$$ These are the first measurements of the channels ηη′ and ωη′ and in almost all the other channels are more precise than previous results. We also obtain, in a more precise fashion, the following ratios of branching ratios:K + K −/π+π−=0.323±0.013, π0η′/π0η=0.548±0.056, ηη′/ηη=0.31±0.15, ωη′/ωη=0.515±0.040, π0η/π0π0=0.303±0.010, ηη/π0π0=0.232±0.011 and π0ω/ηω=0.377±0.12. The measurements are made for different η and η′ decays, and we thus obtain Γη→3π 0/Γη→γγ=0.841±0.034, and $$\Gamma _{\eta ' \to \gamma \gamma } /\Gamma _{\eta ' \to \pi ^0 \pi ^0 \eta } = 0.091 \pm 0.009$$ .
year | journal | country | edition | language |
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1993-01-01 | Zeitschrift für Physik C Particles and Fields |