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The (3He,t) reaction at intermediate energies: Spin-isospin transitions to states in 12N and 13N

Authors :
T. Hennino
C. Gaarde
Clive Ellegaard
J.C. Jourdain
Didier Contardo
P. Radvanyi
A. Guichard
J.S. Larsen
R. Haroutunian
Lars Carlén
J. L. Boyard
I. Bergqvist
M. Roy-Stephan
C. D. Goodman
M. Bedjidian
M. Boivin
J.-Y. Grossiord
A. Brockstedt
Bo Jakobsson
L.P. Ekström
D. Bachelier
J.R. Pizzi
Institut de Physique Nucléaire de Lyon (IPNL)
Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL)
Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)
ALICE
Institut de Physique des 2 Infinis de Lyon (IP2I Lyon)
Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Claude Bernard Lyon 1 (UCBL)
Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Claude Bernard Lyon 1 (UCBL)
Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS)
Institut de Physique Nucléaire d'Orsay (IPNO)
Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11)
Source :
Nuclear Physics A, Nuclear Physics A, Elsevier, 1987, 469, pp.648-668. ⟨10.1016/0375-9474(87)90019-4⟩
Publication Year :
1987
Publisher :
Elsevier BV, 1987.

Abstract

The (3He, t) reaction has been studied at intermediate energies, 600 MeV–2.3 GeV. The reaction is a single-step direct reaction, and the angular distributions are well described by DWIA calculations. At these energies the σρ component of the interaction dominates. The ratio of the isovector strengths ¦J σρ / ρ ¦ derived from the data on 13C appears to remain roughly constant in the energy range 300–700 MeV per nucleon. The triton spectra exhibit a prominent quasi-free peak. The data at momentum transfers q ⪢ 1.7 fm−1 show a shift of the peak towards smaller energy loss than observed in (e, e') experiments at corresponding four-momentum transfers. The shift becomes progressively larger with increasing q and is about 45 MeV at q = 2.5 fm−1. The shift may be caused by particle-hole correlations in the spin-longitudinal channel.

Details

ISSN :
03759474
Volume :
469
Database :
OpenAIRE
Journal :
Nuclear Physics A
Accession number :
edsair.doi.dedup.....1aa7ad1f588c728e0fa0d9607deae336
Full Text :
https://doi.org/10.1016/0375-9474(87)90019-4