Fission of heavy hypernuclei formed in antiproton annihilation
Author(s) -
T. A. Armstrong,
J.P. Bocquet,
G. Ericsson,
T. Johansson,
T. Krogulski,
R. A. Lewis,
F. Malek,
MarieChristine Maurel,
E. Monnand,
J. Mougey,
H. Nifenecker,
J. Passaneau,
Paul B. Perrin,
S.M. Polikanov,
M. Rey-Campagnolle,
C. Ristori,
G. A. Smith,
G. Tibell
Publication year - 1993
Publication title -
physical review c
Language(s) - English
Resource type - Journals
eISSN - 1089-490X
pISSN - 0556-2813
DOI - 10.1103/physrevc.47.1957
Subject(s) - physics , antiproton , fission , annihilation , nuclear physics , multiplicity (mathematics) , recoil , hyperon , lambda , particle physics , atomic physics , hadron , neutron , proton , quantum mechanics , mathematical analysis , mathematics
Heavy hypernuclei are produced in the annihilation of antiprotons in [sup 238]U. The delayed fission of heavy hypernuclei and hypernuclei of fission fragments are observed by using the recoil-distance method in combination with measurement of secondary electron multiplicity. The lifetime of hypernuclei in the region of uranium is found to be (1.25[plus minus]0.15)[times]10[sup [minus]10] sec. It is observed that [Lambda] hyperons predominantly stick to the heavier fission fragments. The yield of hypernuclei is found to be (7.4[plus minus]1.7)[times]10[sup [minus]3] per stopped antiproton. No coincidences with [ital K][sup +] were found. Statistical and systematic errors on the number of events expected do not rule out this possibility.
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