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Fission fragment mass distributions in reactions populating Pb200

A. Chaudhuri, A. Sen, T. K. Ghosh, K. Banerjee, Jhilam Sadhukhan, S. Bhattacharya, P. Roy, T. Roy, C. Bhattacharya, Md. A. Asgar, A. Dey, S. Kundu, S. Manna, J. K. Meena, G. Mukherjee, R. Pandey, T. K. Rana, V. Srivastava, R. Dubey, Gurpreet Kaur, N. Saneesh, P. Sugathan, and P. Bhattacharya
Phys. Rev. C 94, 024617 – Published 24 August 2016

Abstract

The fission fragment mass distributions have been measured in the reactions O16+W184 and F19+Ta181 populating the same compound nucleus Pb200* at similar excitation energies. It is found that the widths of the mass distributions increase monotonically with excitation energy, indicating the absence of quasifission for both reactions. This is contrary to two recent claims of the presence of quasifission in the above-mentioned reactions.

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  • Received 8 April 2016
  • Revised 14 July 2016

DOI:https://doi.org/10.1103/PhysRevC.94.024617

©2016 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

Authors & Affiliations

A. Chaudhuri1, A. Sen1, T. K. Ghosh1,*, K. Banerjee1, Jhilam Sadhukhan1, S. Bhattacharya1, P. Roy1, T. Roy1, C. Bhattacharya1, Md. A. Asgar1, A. Dey1, S. Kundu1, S. Manna1, J. K. Meena1, G. Mukherjee1, R. Pandey1, T. K. Rana1, V. Srivastava1, R. Dubey2, Gurpreet Kaur2, N. Saneesh3, P. Sugathan3, and P. Bhattacharya4

  • 1Variable Energy Cyclotron Centre, 1/AF Bidhan Nagar, Kolkata 700064, India
  • 2Department of Physics, Panjab University, Chandigarh 160014, India
  • 3Inter University Accelerator Centre, Aruna Asaf Ali Marg, New Delhi 110067, India
  • 4Saha Institute of Nuclear Physics, 1/AF Bidhan Nagar, Kolkata 700064, India

  • *tilak@vecc.gov.in

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Issue

Vol. 94, Iss. 2 — August 2016

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Images

  • Figure 1
    Figure 1

    Folding angle distributions of complementary fission fragments for the system F19+Ta181 at an excitation energy of 65 MeV. The rectangle indicates the gate used to select the fusion fission events for mass determination.

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  • Figure 2
    Figure 2

    Experimental mass distributions of fission fragments for the reactions F19+Ta181 [(a)–(d)] and O16+W184 [(e)–(h)] at different excitation energies. They were fitted by a single Gaussian, shown by full (red) lines.

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  • Figure 3
    Figure 3

    Variation of the standard deviation σm(u) of the fitted symmetric mass distribution with excitation energy. The calculated widths are shown in (blue) dashed line, the shaded region indicates uncertainties in calculation (see text). The predicted [8] variation of the sum of the fast fission and quasifission cross sections (normalized with respect to the fusion cross sections) with excitation energy are presented in the inset.

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  • Figure 4
    Figure 4

    Variation of the ratio of the experimental (measured) and theoretically calculated standard deviation σm(u) of the fitted symmetric mass distribution with c.m. energy. The Coulomb barriers for the F19+Ta181 (77.8 MeV) and O16+W184 (71 MeV) reactions are shown by arrows. The dashed line (constant value = 1) is a guide to the eye.

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  • Figure 5
    Figure 5

    Measured mass angle distributions of the fission fragments in the reaction F19+Ta181 at an excitation energy of 75.9 MeV.

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