corner
corner

Phys. Rev. C 60, 064003 (1999) [14 pages]

Determination of the asymptotic D- to S-state ratio for 6Li via (6Li→,d) transfer reactions

Download: PDF (214 kB) Buy this article Export: BibTeX or EndNote (RIS)

K. D. Veal1,2,*, C. R. Brune1,2, W. H. Geist1,2,*, H. J. Karwowski1,2, E. J. Ludwig1,2, E. E. Bartosz3, P. D. Cathers3, T. L. Drummer3,†, K. W. Kemper3, A. M. Eiró4, F. D. Santos4, B. Kozlowska2,5, H. J. Maier6, and I. J. Thompson7
1Department of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, North Carolina 27599-3255
2Triangle Universities Nuclear Laboratory, Durham, North Carolina 27788-0308
3Department of Physics, Florida State University, Tallahassee, Florida 32306-4350
4Departamento de Fisica and Centro de Fisica Nuclear da Universidade de Lisboa, Lisboa, Portugal
5Institute of Physics, University of Silesia, Katowice, Poland
6University of Munich, Garching, Germany
7Department of Physics, University of Surrey, Guildford GU2 5XH, United Kingdom

Received 19 July 1999; published 16 November 1999

Measurements of cross section, vector analyzing power Ay, and tensor analyzing powers Azz and Axz over the angular range 10°<~θlab<~40° have been performed at E(6Li)=34MeV for the 58Ni(6Li→,d)62Zn and 40Ca(6Li→,d)44Ti reactions leading to the ground state and first excited state of both residual nuclei. The reactions are described by distorted-wave Born approximation calculations, assuming a direct α-particle transfer mechanism. The asymptotic D/S state ratio η for the d+α relative wave function in 6Li is determined. In this one-step analysis, the best fit to the tensor observables leads to a value of η=+0.0003±0.0009. This value is in disagreement with most of the previous theoretical and empirical determinations of η. An investigation of two-step reaction mechanisms is performed, allowing the Jπ=3+, 2+, and 1+ states in 6Li to contribute to the transfer reaction channel. Reasonable agreement is achieved with the cross section and vector analyzing power data for several possible two-step amplitudes. It is found that the fitted magnitude of η increases with increasing two-step amplitude, giving η=-0.0030±0.0022 for unit amplitude, therefore not changing significantly from our one-step result.

© 1999 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.60.064003
DOI:
10.1103/PhysRevC.60.064003
PACS:
21.45.+v, 24.70.+s, 25.70.Hi, 24.50.+g

*Present adddress: Los Alamos National Laboratory, Los Alamos, NM 87545.

Present address: University of Illinois, Urbana, IL 61800.