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Phys. Rev. Lett. 100, 042501 (2008) [4 pages]

First Measurement of the Giant Monopole and Quadrupole Resonances in a Short-Lived Nucleus: 56Ni

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C. Monrozeau1, E. Khan1, Y. Blumenfeld1, C. E. Demonchy2, W. Mittig3, P. Roussel-Chomaz3, D. Beaumel1, M. Caamaño4, D. Cortina-Gil4, J. P. Ebran1, N. Frascaria1, U. Garg5, M. Gelin3, A. Gillibert6, D. Gupta1,*, N. Keeley6, F. Maréchal1, A. Obertelli6, and J-A. Scarpaci1
1Institut de Physique Nucléaire IN2P3/CNRS, Université Paris Sud, 91406 Orsay Cedex, France
2Department of Physics, Olivier Lodge Laboratory, University of Liverpool, Liverpool L69 7ZE, United Kingdom
3GANIL, DSM/CEA, IN2P3/CNRS, BP 5027, 14076 Caen Cedex 5, France
4Universidad Santiago de Compostela, E-15706 Santiago de Compostela, Spain
5Physics Department, University of Notre Dame, Notre Dame, Indiana 46556, USA
6CEA/DSM/DAPNIA/SPhN, Saclay, 91191 Gif-sur-Yvette Cedex, France

Received 19 July 2007; published 28 January 2008

The isoscalar giant monopole resonance (GMR) and giant quadrupole resonance (GQR) have been measured in the 56Ni unstable nucleus by inducing the 56Ni(d,d) reaction at 50A  MeV in the Maya active target at the GANIL facility. The GMR and GQR centroids are measured at 19.3±0.5  MeV and 16.2±0.5  MeV, respectively. The corresponding angular distributions are extracted from 3° to 7°. A multipole decomposition analysis using distorted wave Born approximation with random phase approximation transition densities shows that both the GMR and the GQR exhaust a large fraction of the energy-weighted sum rule. The demonstration of this new method opens a broad range of giant resonance studies at intermediate-energy radioactive beam facilities.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.100.042501
DOI:
10.1103/PhysRevLett.100.042501
PACS:
24.30.Cz, 21.10.Re, 24.50.+g, 27.40.+z

*Present address: Variable Energy Cyclotron Centre, 1/AF Bidhan Nagar, Kolkata 700064, India