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Phi pi0 and Phi eta production in anti-proton annihilation at rest in a hydrogen gas target at NTP

Academic Article
Publication Date:
1995
abstract:
Data of antiproton annihilation at rest in a hydrogen gas target at NTP have been collected with the Obelix spectrometer exposed to the beam extracted from the LEAR accelerator of CERN. The reactions pbar p --> Phi pi0 and Phi Eta have been studied. The analysis of the angular distribution of the kaons emitted by the ~b decay has shown that the reaction ~p ~ ¢~" 0 occurs essentially from 3S 1 states with a production rate RrcrP = (2.46 ___ 0.23 _ 0.07) x 10 -4, while the rate from 1P 1 states is compatible with zero. Because of acceptance limitations, 3S 1 and 1p1 contributions to the reaction ~p ~ ~br/could not be resolved and lower and upper limits for the production rate have been measured with the middle value Rm. P = (0.87 + 0.21) x 10 -4. Also, for the phase-space K+K-r/ events the production rate RN~ = (4.67 ___ 0.35) × 10 -4 has been measured. The thTr ° and th*/branching ratios in S- and P-waves (defined in the text) have been estimated in a model dependent way. For the evaluation of the ~b~/ rate, a combination of our production rate and of data obtained with a liquid target has been used. The ~b~r ° production rate, compared to our preliminary value for the to~ -° production, confirms the strong violation of the OZI rule observed in other experiments. No violation is apparent in the PhiEta production.
Iris type:
1.1 Articolo in rivista
List of contributors:
V. G. Ableev a. i. M., Agnello b; F., Balestra c; G., Bendiscioli e; S., Bergamaschi e; A. Bertin e. E., Botta c; T., Bressani c; M., Bruschi e; M. P., Bussa c; L., Busso c; D., Calvo b; M. Capponi f. C., Cavion a; B., Cereda f; P. Cerello, C.; C., Cical6 h; M. Corradini d., ~.; S., Costa c; S., De Castro e; Denisov g, O. Y. u.; F., D'Isep c; A. Donzella d. L., Fava c; A. Feliciello c. L. Ferrero c. A. Filippi c. V., Filippini e; Fontana, Andrea; D., Galli ~; R., Garfagnini c; U., Gastaldi a; B., Giacobbe f; P., Gianotti i; O. E., Gorchakov g; A., Grasso c; C., Guaraldo i; F., Iazzi b; A., Lanaro i; E., Lodi Rizzini d; M. Lombardi a. V., Lucherini i; A., Maggiora c; S., Marcello c; U., Marconi e; G. V., Margagliotti J; A., Masoni h; B., Minetti b; Montagna, PAOLO MARIA; M., Morando k; F., Nichitiu i; L, ; D., Panzieri c; D., Parena e; P., Pauli J; C., Petrascu i; 2, ; M., Piccinini f; S., Prakhov g; G., Puddu h; A., Rosca i; 2, ; E., Rossetto; Rotondi, Alberto; A. M., Rozhdenstvensky g; A., Saino e; P., Salvini e; L., Santi 1; M. G., Sapozhnikov g; C., Scoglio e; N., Semprini Cesari f; S., Serci h; R., Spighi f; P., Temnikov h; S., Tessaro J; F., Tosello c; V. I., Tretyak g; G. L., Usai h; L., Vannucci a; S., Vecchi f; G., Vedovato a; L., Venturelli d; M., Villa f; A., Vitale f; A. Zenoni r. e., N.; A. Zoccoli, F.
Authors of the University:
FONTANA ANDREA
MONTAGNA PAOLO MARIA
Handle:
https://iris.unipv.it/handle/11571/446051
Published in:
NUCLEAR PHYSICS. A
Journal
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