Antiproton-proton annihilation at rest intoπ + π − η ′ andπ + π − η from atomicS andP states
Autor: | H. Nguyen, W. Dahme, C. Laa, H. Vonach, U. Schaefer, J. Jeanjean, H. Kalinowsky, J. Reifenröther, U. Gastaldi, M. Heel, P. Weidenauer, S. Barlag, M. Comyn, Glenn M. Marshall, G. A. Beer, U. Straumann, Claude Amsler, M. Botlo, K. D. Duch, J.C. Bizot, B. Howard, D. Bailey, M. Ziegler, B. May, Eberhard Klempt, B. Delcourt, Shama Ahmad, R. Howard, M. Doser, L. P. Robertson, F. Feld-Dahme, R. Landua, F. Kayser, E.G. Auld, W. R. Wodrich, O. Schreiber, K. L. Erdman, B. L. White, J. Riedlberger, C. Sabev, J. N. Butler, P. Truöl, D. Axen |
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Rok vydání: | 1990 |
Předmět: | |
Zdroj: | Zeitschrift für Physik C Particles and Fields. 47:353-365 |
ISSN: | 1434-6052 0170-9739 |
DOI: | 10.1007/bf01565858 |
Popis: | 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. $$\begin{gathered} BR(S - wave \to \pi ^ + \pi ^ - \eta ) = (13.7 \pm 1.46) \cdot 10^{ - 3} \hfill \\ BR(P - wave \to \pi ^ + \pi ^ - \eta ) = (3.35 \pm 0.84) \cdot 10^{ - 3} \hfill \\ BR(S - wave \to \pi ^ + \pi ^ - \eta ') = (3.46 \pm 0.67) \cdot 10^{ - 3} \hfill \\ BR(P - wave \to \pi ^ + \pi ^ - \eta ') = (0.61 \pm 0.33) \cdot 10^{ - 3} . \hfill \\ \end{gathered} $$ |
Databáze: | OpenAIRE |
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