S. R. Banerjee
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Physical Review C | 2008
Srijit Bhattacharya; S. Mukhopadhyay; Deepak Pandit; S. K. Pal; A. De; S. Bhattacharya; C. Bhattacharya; K. Banerjee; S. Kundu; A. Dey; G. Mukherjee; T. K. Ghosh; D. Gupta; S. R. Banerjee; Af Bidhan Nagar
High energy {gamma} rays in coincidence with low energy yrast {gamma} rays have been measured from {sup 113}Sb, at excitation energies of 109 and 122 MeV, formed by bombarding {sup 20}Ne on {sup 93}Nb at projectile energies of 145 and 160 MeV, respectively, to study the role of angular momentum (J) and temperature (T) over giant dipole resonance (GDR) width ({gamma}). The maximum populated angular momenta for fusion were 67({Dirac_h}/2{pi}) and 73({Dirac_h}/2{pi}), respectively, for the above-mentioned beam energies. The high energy photons were detected using a Large Area Modular BaF{sub 2} Detector Array (LAMBDA) along with a 24-element multiplicity filter. After pre-equilibrium corrections, the excitation energy E* was averaged over the decay steps of the compound nucleus (CN). The average values of temperature, angular momentum, CN mass, etc., have been calculated using the statistical model code CASCADE. Using those average values, results show the systematic increase of GDR width with T, which is consistent with Kusnezov parametrization and the thermal shape fluctuation model (TSFM). The rise of GDR width with temperature also supports the assumptions of adiabatic coupling in the TSFM. But the GDR widths and corresponding reduced plots with J are not consistent with those of the theoretical modelmorexa0» at high spins.«xa0less
Physical Review C | 2013
Deepak Pandit; Balaram Dey; Debasish Mondal; S. Mukhopadhyay; S. K. Pal; Srijit Bhattacharya; A. De; S. R. Banerjee
The first systematic study of the correlation between the experimental giant dipole resonance (GDR) width and the average deformation � β� of the nucleus at finite excitation is presented for the mass region A ∼ 59 to 208. We show that the width of the GDR (� ) and the quadrupole deformation of the nucleus do not follow a linear relation, as predicted earlier, owing to the GDR-induced quadrupole moment, and the correlation also depends on the mass of the nuclei. The different empirical values of � β� extracted from the experimental GDR width match exceptionally well with the thermal shape fluctuation model. As a result, this universal correlation between
Physical Review C | 2013
H. Pai; G. Mukherjee; S. Bhattacharya; C. Bhattacharya; S. Bhattacharyya; T. Bhattacharjee; Somen Chanda; S. Rajbanshi; A. Goswami; M. Gohil; S. Kundu; T. K. Ghosh; K. Banerjee; T. K. Rana; R. Pandey; G. K. Prajapati; S. R. Banerjee; S. Mukhopadhyay; Deepak Pandit; S. K. Pal; J. K. Meena; P. Mukhopadhyay; A. Choudhury
The excited states in the odd-
international conference on management of innovation and technology | 2000
R. Aganwal; Balaram Ghosh; S. R. Banerjee; S. Kishore Pal
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Physical Review C | 2017
Deepak Pandit; Debasish Mondal; Balaram Dey; Srijit Bhattacharya; S. Mukhopadhyay; S. K. Pal; A. De; S. R. Banerjee
2017 8th Annual Industrial Automation and Electromechanical Engineering Conference (IEMECON) | 2017
Himadri Nath Saha; Supratim Auddy; Subrata Pal; Shubham Kumar; Shivesh Pandey; Rakhee Singh; Amrendra Kumar Singh; S. R. Banerjee; Debmalya Ghosh; Sanhita Saha
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Physical Review C | 2015
D. Banerjee; Archita Saha; T. Bhattacharjee; R. Guin; P. Das; Deepak Pandit; Avinandan Mukherjee; Anindita Chowdhury; S. Bhattacharya; S. Das Gupta; S. Bhattacharyya; P. Mukhopadhyay; S. R. Banerjee
Tl nucleus have been studied by populating them using the
Physical Review C | 2013
A. Ray; A. De; S. Kailas; S. R. Banerjee; K. Banerjee; S. Saha; A. Chatterjee
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Archive | 2018
S Majumder B Saha S Kumar; S. R. Banerjee
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2017 8th Annual Industrial Automation and Electromechanical Engineering Conference (IEMECON) | 2017
Himadri Nath Saha; Supratim Auddy; Subrata Pal; Shubham Kumar; Subhadeep Jasu; Rp Singh; Rakhee Singh; S. R. Banerjee; Priyanshu Sharan; Ankita Maity
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