6533b85bfe1ef96bd12ba92b

RESEARCH PRODUCT

Antiproton-proton annihilation at rest intoπ + π − η ′ andπ + π − η from atomicS andP states

H. NguyenW. DahmeC. LaaH. VonachU. SchaeferJ. JeanjeanH. KalinowskyJ. ReifenrötherU. GastaldiM. HeelP. WeidenauerS. BarlagM. ComynGlenn M. MarshallG. A. BeerU. StraumannClaude AmslerM. BotloK. D. DuchJ.c. BizotB. HowardD. BaileyM. ZieglerB. MayEberhard KlemptB. DelcourtShama AhmadR. HowardM. DoserL. P. RobertsonF. Feld-dahmeR. LanduaF. KayserE.g. AuldW. R. WodrichO. SchreiberK. L. ErdmanB. L. WhiteJ. RiedlbergerC. SabevJ. N. ButlerP. TruölD. Axen

subject

Nuclear physicsPhysicsPionAnnihilationPhysics and Astronomy (miscellaneous)AntiprotonBranching fractionAnalytical chemistryEngineering (miscellaneous)

description

We have measured the branching ratios for\(\bar pp\) annihilation at rest intoπ+π−η andπ+π−η′ in hydrogen gas in two data samples that have different fractions ofS-wave andP-wave initial states. The branching ratios are derived from a comparison with the topological branching ratio for\(\bar pp\) annihilations into four charged pions of (49±4)% and the branching ratio intoπ+π−π+π−π0 of (18.7±1.6)%. We find a significant reduction of the branching ratios fromP-states for\(\bar pp \to \pi ^ + \pi ^ - \eta \) andπ+π−η′ in comparison toS-state annihilation. $$\begin{gathered} BR(S - wave \to \pi ^ + \pi ^ - \eta ) = (13.7 \pm 1.46) \cdot 10^{ - 3} \hfill \\ BR(P - wave \to \pi ^ + \pi ^ - \eta ) = (3.35 \pm 0.84) \cdot 10^{ - 3} \hfill \\ BR(S - wave \to \pi ^ + \pi ^ - \eta ') = (3.46 \pm 0.67) \cdot 10^{ - 3} \hfill \\ BR(P - wave \to \pi ^ + \pi ^ - \eta ') = (0.61 \pm 0.33) \cdot 10^{ - 3} . \hfill \\ \end{gathered} $$

https://doi.org/10.1007/bf01565858