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No signature of the saturation of giant dipole resonance width in medium-mass nuclei

S. Mukhopadhyay1,2,*, Pratap Roy1,2,†, Debasish Mondal1, Deepak Pandit1,2, Surajit Pal1, Balaram Dey3, Srijit Bhattacharya4, A. De5, T. K. Rana1,2 et al.

S. Kundu1,2, J. Sadhukhan1,2, C. Bhattacharya1,2, and S. R. Banerjee1

  • 1Variable Energy Cyclotron Centre, 1/AF-Bidhannagar, Kolkata 700064, India
  • 2Homi Bhabha National Institute, Training School Complex, Anushaktinagar, Mumbai 400094, India
  • 3Department of Physics, Bankura University, Bankura 722155, India
  • 4Department of Physics, Barasat Government College, Barasat, N 24 Pgs, Kolkata 700124, India
  • 5Department of Physics, Raniganj Girls' College, Raniganj 713358, India

  • *supm@vecc.gov.in
  • †Present address: GSI Helmholtzzentrum für Schwerionenforschung, D-64291 Darmstadt, Germany.

Phys. Rev. C 104, L031304 – Published 13 September, 2021

DOI: https://doi.org/10.1103/PhysRevC.104.L031304

Abstract

An experimental study on the temperature (T) dependence of giant dipole resonance (GDR) width was performed for the medium mass nucleus Kr74 in the range of T≈2–2.5 MeV at an average angular momentum of 26ℏ using the O16+Ni58 fusion reaction. The emitted high-energy γ rays and evaporated neutrons were measured in coincidence with low-energy discrete γ-ray multiplicities. The GDR parameters, nuclear level density parameter, and nuclear temperature were determined by the statistical model analysis of the high-energy γ-ray spectra as well as evaporated neutron spectra. The measured GDR width is found to increase monotonically with temperature, in contradiction with the recent observation of the width saturation in Mo88. Comparisons of the measured data with predictions of the adiabatic thermal shape fluctuation model and its refined version, the critical temperature included fluctuation model, are presented and discussed.

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