corner
corner

Phys. Rev. C 80, 024319 (2009) [13 pages]

Polarization transfer measurements for 12C(p⃗,n⃗)12N(g.s.,1+) at 296 MeV and nuclear correlation effects

Download: PDF (2,225 kB) Buy this article Export: BibTeX or EndNote (RIS)

M. Dozono1,*, T. Wakasa1, E. Ihara1, S. Asaji1, K. Fujita1, K. Hatanaka2, M. Ichimura3, T. Ishida4, T. Kaneda2, H. Matsubara2, Y. Nagasue1, T. Noro1, Y. Sakemi4, Y. Shimizu5, H. Takeda1, Y. Tameshige2, A. Tamii2, and Y. Yamada1
1Department of Physics, Kyushu University, Higashi, Fukuoka 812-8581, Japan
2Research Center for Nuclear Physics, Osaka University, Ibaraki, Osaka 567-0047, Japan
3Faculty of Computer and Information Sciences, Hosei University, Koganei, Tokyo 184-8584, Japan
4Cyclotron and Radioisotope Center, Tohoku University, Aoba, Miyagi 980-8578, Japan
5Center for Nuclear Study, The University of Tokyo, Bunkyo, Tokyo 113-0033, Japan

Received 24 March 2009; published 31 August 2009

Differential cross sections and complete sets of polarization observables are presented for the Gamow-Teller 12C(p⃗,n⃗)12N(g.s.,1+) reaction at a bombarding energy of 296 MeV with momentum transfers q of 0.1 to 2.2fm-1. The polarization transfer observables are used to deduce the spin-longitudinal cross section, IDq, and spin-transverse cross sections, IDp and IDn. The data are compared with calculations based on the distorted-wave impulse approximation (DWIA) using shell-model wave functions. Significant differences between the experimental and theoretical results are observed for all three spin-dependent IDi at momentum transfers of q≳0.5fm-1, suggesting the existence of nuclear correlations beyond the shell model. We also performed DWIA calculations employing random-phase approximation (RPA) response functions and found that the observed discrepancy is partly resolved by the pionic and ρ-mesonic correlation effects.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.80.024319
DOI:
10.1103/PhysRevC.80.024319
PACS:
24.70.+s, 25.40.Kv, 27.20.+n