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Survival of orbiting in Ne20 (7–10 MeV/nucleon) + C12 reactions

C. Bhattacharya, A. Dey, S. Kundu, K. Banerjee, S. Bhattacharya, S. Mukhopadhyay, D. Gupta, T. Bhattacharjee, S. R. Banerjee, S. Bhattacharyya, T. Rana, S. K. Basu, R. Saha, S. Bhattacharjee, K. Krishan, A. Mukherjee, D. Bandopadhyay, and C. Beck
Phys. Rev. C 72, 021601(R) – Published 25 August 2005

Abstract

The inclusive energy distributions of fragments with Z 3 emitted from the bombardment of C12 by Ne20 beams with incident energies between 145 and 200 MeV have been measured in the angular range θlab~10°50°. Damped fragment yields in all cases have been found to be characteristic of emission from fully energy equilibrated composites; for B and C fragments, average Q values, Q, were independent of the center-of-mass emission angle (θc.m.), and the angular distributions followed a ~1/sinθc.m.-like variation, signifying long lifetimes of the emitting dinuclear systems. Estimates of total yields of these fragments have been found to be much larger than those predicted by the standard statistical model. This may be indicative of the survival of an orbiting-like process in the C12+Ne20 system at these energies.

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  • Received 22 February 2005

DOI:https://doi.org/10.1103/PhysRevC.72.021601

©2005 American Physical Society

Authors & Affiliations

C. Bhattacharya, A. Dey, S. Kundu, K. Banerjee, S. Bhattacharya, S. Mukhopadhyay, D. Gupta*, T. Bhattacharjee, S. R. Banerjee, S. Bhattacharyya, T. Rana, S. K. Basu, R. Saha, S. Bhattacharjee, K. Krishan, A. Mukherjee, and D. Bandopadhyay§

  • Variable Energy Cyclotron Centre, Sector 1, Block AF, Bidhan Nagar, Kolkata 700 064, India

C. Beck

  • Institut de Recherches Subatomiques, UMR7500, CNRS-IN2P3 and Université Louis Pasteur, 23 Rue du Loess, Bôite Postale 28, F-67037 Strasbourg Cedex 2, France

  • *Present address: Institut de Physique Nucleaire, CNRS-IN2P3, F-91406 Orsay Cedex, France.
  • Present address: 306, VIP Enclave, VIP Road, Kolkata 700 059, India.
  • Present address: Saha Institute of Nuclear Physics, 1/AF Bidhan Nagar, Kolkata 700 064, India.
  • §Present address: Department of Physics, University of Guelph, Guelph, Ontario N1G 2W1, Canada.

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Issue

Vol. 72, Iss. 2 — August 2005

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Images

  • Figure 1
    Figure 1
    Measured energy distributions of the B and C fragments emitted in the reaction Ne20 + 12C at Elab= 145, 158, 168, 178, and 200 MeV (from top to bottom, respectively). The arrow corresponds to the position of the peak of the Gaussian distribution.Reuse & Permissions
  • Figure 2
    Figure 2
    The c.m. angular distributions of the B and C fragments obtained at Elab= 145, 158, 168, 178, and 200 MeV (from (a) to (e), respectively). Solid circles correspond to experimental data and the solid curves are f(θc.m.) ∼ 1/sinθc.m. fit to the data.Reuse & Permissions
  • Figure 3
    Figure 3
    Average Q values of the B and C fragments obtained at Elab= 145, 158, 168, 178, and 200 MeV (denoted by inverted triangle square, diamond, triangle, and circle, respectively) plotted as a function of c.m. emission angle.Reuse & Permissions
  • Figure 4
    Figure 4
    The excitation functions for the angle-integrated yield of the carbon and boron fragments. Triangles are the present data; lower energy data (shown by solid points) have been taken from [8]. In the left side of the figure, solid, dashed and dash-dot-dotted curves are the predictions of the statistical model with l=lcr,l=lgr, and the equilibrium orbiting model, respectively. Solid curves in the right side of the figure are EHFM predictions.Reuse & Permissions
  • Figure 5
    Figure 5
    Bombarding energy dependence of the average Q values. The solid line shows the linear dependence of Q with bombarding energy. The Q values at lower energies are taken from [9].Reuse & Permissions
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