Phys. Rev. C 67, 024606 (2003) [12 pages]

Structure of the 10Li nucleus investigated via the 9Li(d,p)10Li reaction

Download: PDF (1410 kB) or Buy this Article (Use Article Pack) Export: BibTeX or EndNote (RIS)

P. Santi *, J. J. Kolata, V. Guimãraes , D. Peterson , R. White-Stevens, and E. Rischette
Physics Department, University of Notre Dame, Notre Dame, Indiana 46556-5670

D. Bazin, B. M. Sherrill, and A. Navin §
National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824-1321

P. A. DeYoung and P. L. Jolivette
Physics Department, Hope College, Holland, Michigan 49422-9000

G. F. Peaslee
Chemistry Department, Hope College, Holland, Michigan 49422-9000

R. T. Guray **
Physics Department, The Ohio State University, Columbus, Ohio 43210

Received 8 July 2002; published 24 February 2003

The structure of the particle unbound nucleus 10Li was investigated in a kinematically complete experiment using the 9Li(d,p)10Li reaction in inverse kinematics at an incident 9Li energy of 20 MeV/nucleon. The experiment utilized the S800 Spectrograph at the National Superconducting Cyclotron Laboratory to measure the outgoing 9Li from the breakup of 10Li in coincidence with the recoiling protons from the (d,p) reaction which were measured using an array of silicon detectors. Based on the kinematics of the recoiling protons from the 9Li(d,p) reaction, we measured a lower limit of Δ=33.10±0.08 MeV (i.e., Δ>33.02 MeV) for the mass excess of 10Li which is consistent with previous measurements. Through the complete reconstruction of the breakup kinematics, the structure of 10Li associated with a ground state 9Li core was distinguishable from structure associated with a 9Li core in its first excited state. The observed ratio of 9Li* core events to the total number of 10Li events that were detected in the experiment was 0.10±0.04 at forward center of mass angles (2.7° to 9.5°), and 0.24±0.03 at more backward center of mass angles (11° to 26°). The resulting Q-value spectra was best fit with either a single resonance located at Q=-2.58(11) MeV [corresponding to a neutron separation energy Sn=-0.35(11) MeV] or two resonances located at Q=-3.00(24) MeV [Sn=-0.77(24) MeV] and Q>-2.43 MeV (Sn>-0.2 MeV).


©2003 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevC.67.024606
DOI: 10.1103/PhysRevC.67.024606
PACS: 21.10.-k, 25.70.Hi, 27.20.+n

* Present address: National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI 48824-1321.
Present address: Instituto de Fisica, Universidade de Sao Paulo, Caixa Postal 66.318 CEP, 05315-970 Sao Paulo, Brazil.
Present address: Department of Chemistry, Oregon State University, Corvallis, OR 97331-5903.
§ Permanent address: Nuclear Physics Division, Bhabha Atomic Research Center, Trombay, Mumbai 400 085, India.
** Present address: Celal Bayar University, Muradiye Campus, Department of Physics, Manisa 45000, Turkey.

[ Abstract  |  Previous article  |  Next article  |  Issue 2 ]