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Phys. Rev. C 48, 118–135 (1993)

Electromagnetic excitation of 11Li

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D. Sackett, K. Ieki, A. Galonsky, C. A. Bertulani, H. Esbensen, J. J. Kruse, W. G. Lynch, D. J. Morrissey, N. A. Orr, B. M. Sherrill, H. Schulz, A. Sustich, and J. A. Winger
National Superconducting Cyclotron Laboratory and Department of Physics Astronomy, Michigan State University, East Lansing, Michigan 48824

F. Deák, Á. Horváth, and Á. Kiss
Department of Atomic Physics, Eötvös University, Puskin utca 5-7, H-1088 Budapest 8, Hungary

Z. Seres
KFKI Research Institute for Particle and Nuclear Physics of the Hungarian Academy of Sciences, H-1525 Budapest 114, Hungary

J. J. Kolata
Department of Physics, University of Notre Dame, Notre Dame, Indiana 46556

R. E. Warner
Department of Physics, Oberlin College, Oberlin, Ohio 44074

D. L. Humphrey
Department of Physics, Western Kentucky University, Bowling Green, Kentucky 42101

Received 30 November 1992; published in the issue dated July 1993

We have performed a kinematically complete measurement of the Coulomb dissociation of 28 MeV/nucleon 11Li into 9Li and two neutrons by a Pb target. From the energies and angles of the emitted neutrons and of 9Li, the excitation energy E of 11Li was determined on an event-by-event basis, and the Coulomb dissociation cross section as a function of excitation energy was constructed. The photonuclear cross section σE1(E) and the dipole strength function dB(E1)/dE were determined from the Coulomb dissociation cross section. σE1(E) has a peak at E=1.0 MeV and a width Γ=0.8 MeV. These parameters are consistent with the picture of a soft dipole mode. However, a significant post-breakup Coulomb acceleration of 9Li suggests instead a direct breakup. The complete kinematical measurement also allowed neutron and 9Li momentum distributions to be constructed in the rest frame of the 11Li. The momentum distributions were fitted with Gaussian functions, yielding width parameters σ9=18±4 MeV/c and σn=13±3 MeV/c. A more general feature of the breakup mechanism of 11Li could be deduced from these measurements. It was found that the 9Li and neutron momentum distributions and the neutron-neutron relative momentum distribution could be reproduced if the 11Li excitation energy was partitioned between the 9Li and the neutrons by a three-body phase space distribution. This indicates there is no directional correlation between the halo neutrons, and shows that the halo neutrons do not exist as a dineutron bound to a 9Li core.

© 1993 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.48.118
DOI:
10.1103/PhysRevC.48.118
PACS:
25.70.De, 21.10.Gv, 25.20.Dc, 25.60.+v