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3–5 Feb 2019
Lipika Auditorium, Visva-Bharati, Santiniketan
Asia/Kolkata timezone

Contribution List

98 / 98
Prof. Biswarup Mukhopadhyaya (Harish-Chandra Research Institute, Allahabad, India)
03/02/2019, 11:30
Prof. Gautam Bhattacharyya (Saha Institute of Nuclear Physics)
03/02/2019, 14:00
Prof. Anindya Datta (University of Calcutta)
04/02/2019, 12:35
Prof. Palash Pal (University of Calcutta)
04/02/2019, 15:50
Prof. S.S. Ghugre (UGC-DAE-Consortium for Scientific Research, Kolkata 700 098, India)
04/02/2019, 17:20
Mr S. Rai1,2 , B. Mukherjee2 , U.S. Ghosh2 , A. Biswas2, A. Chakraborty2, A.K. Mondal2, S. Chakraborty3 , G. Mukherjee4 , I. Bala5 , S. Muralithar5 , and R.P. Singh5 (1Department of Physics, Salesian College, Siliguri Campus, Siliguri - 734001, India. 2Department of Physics, Siksha-Bhavana, Visva-Bharati, Santiniketan, Bolpur - 731235, India. 3Department of Physics, Institute of Science, Banaras Hindu University, Varanasi - 221005, India. 4Variable Energy Cyclotron Centre, 1/AF Bidhannagar, Kolkata - 700064, India. 5Inter University Accelerator Centre, Aruna Asaf Ali Marg, New Delhi - 110067, India. )

Excited high spin states in 66Zn, populated in the fusion evaporation reaction 52Cr(18O, 2p2n), have been studied using in-beam γ-spectroscopic methods. The Indian National Gamma-ray Array (INGA) equipped with fourteen Compton suppressed Hp-Ge clover detectors was used to detect the gamma-rays emitted by the de-exciting nucleus. The 18O beam at 72.5 MeV was supplied by the 15UD Pelletron...

Mr Aniruddha Dey 1,2 *, S. Mukhopadhyay 1 , D. C. Biswas 1 , A. Chakraborty 2 , A. K. Mondal 2 , K. Mondal 2 , B. N. Joshi 1 , S. Chatterjee 3 , S. Samanta 3 , S. Das 3 , Soumik Bhattacharya 4 , R. Banik 4 , S. Nandi 4 , R. Raut 3 , G. Mukherjee 4 , S. Bhattacharyya 4 , S. S. Ghugre 3 , and A. Goswami 5 (1Nuclear Physics Division, Bhabha Atomic Research Centre, Mumbai 400085, India 2Department of Physics, Visva Bharati University, Shantiniketan, Birbhum, 731236, West Bengal, India 3UGC-DAE CSR, Kolkata Centre, Kolkata 700098, India 4Variable Energy Cyclotron Centre, 1/AF Bidhan Nagar, Kolkata 700064, India and 5Saha Institute of Nuclear Physics, Kolkata 700064, India *Email: deyaniruddha07@gmail.com )

The data for the work has been obtained from the experiment performed at Variable
Energy Cyclotron Centre, Kolkata using the INGA facility. A self-supporting 232Th target
of thickness ~25 mg/cm2 was bombarded with 30 MeV α particles. A total of six
compton suppressed clover Ge detectors and one LEPS detector were used in the
array.
By analyzing the two-fold coincidence data, a complete...

Mr A.K. Mondal1,2, S. Mukhopadhyay1 , A. Chakraborty2 , D.C. Biswas1 , L.S. Danu1 , A. Blanc3 , G. de France4 , M. Jentschel3 , U. Köster3 , S. Leoni5 , P. Mutti3 , G. Simpson6 , T. Soldner3 , C. A. Ur7 , and W. Urban (1 Nuclear Physics Division, Bhabha Atomic Research Centre, Trombay, Mumbai - 400 085 2 Department of Physics, Siksha- Bhavana, Visva-Bharati, Santiniketan - 731 235 3 ILL, 71 Avenue des Martyrs, 38042 Grenoble CEDEX 9, France 4 GANIL, BP 55027, F-14076 Caen Cedex 5, France 5 Università degli Studi di Milano, I-20133 Milano, Italy 6 LPSC, 53 Avenue des Martyrs, 38026 Grenoble, France 7 INFN Sezione di Padova, I-35131 Padova, Italy and 8 Faculty of Physics, University of Warsaw, PL 02-093 Warszawa, Poland )

Neutron-rich nuclei in the mass region A~100 exhibit large variety of interesting nuclear
structure phenomena. The nuclei having neutron number N ≤ 58 has a nearly spherical ground
state, but they undergo a rapid shape transition from nearly spherical to well-deformed prolate
deformation as N = 60 is approached. This abrupt shape change was correctly described by largescale Monte Carlo shell...

Mrs A. Sharma1, Shashi. K. Dhiman1, Pankaj Kumar1, S. Muralithar2, R. P. Singh2, Yashraj2, K. Katre2, R. K. Gurjar2, S. S. Tiwary3, Neelam4, Anuj4 , S. Kumar4, S. Suman5, S. K. Tandel5, R. Raut 6, Sutanu Bhattacharya7, Umakant Lamani8, Subodh 9 (1Department of Physics, Himachal Pradesh University, Shimla 171005,India. 2India. Inter University Accelerator Centre, Aruna Asaf Ali Marg, New Delhi 110067, India. 3Department of Physics, Institute of Science, Banaras Hindu University, Varanasi 221005, India 4 Department of Physics and Astrophysics, University of Delhi, New Delhi 110007, India. 5UM-DAE Centre for Excellence in Basic Sciences, Mumbai 400098, India. 6UGC-DAE Consortium for Scientific Research, Kolkata Centre, Kolkata 700098, India. 7Department of Pure and Applied Physics, Guru Ghasidas Viswavidyalaya, Koni, Bilaspur 495009,India. 8Department of Physics, Indian Institute of Technology Bombay, Powai, Mumbai,400076, India. 9Department of Physics, Panjab University, Chandigarh, India. of Physics, Himachal Pradesh University, Shimla 171005,India. 2India. Inter University Accelerator Centre, Aruna Asaf Ali Marg, New Delhi 110067, India. 3Department of Physics, Institute of Science, Banaras Hindu University, Varanasi 221005, India 4 Department of Physics and Astrophysics, University of Delhi, New Delhi 110007, India. 5UM-DAE Centre for Excellence in Basic Sciences, Mumbai 400098, India. 6UGC-DAE Consortium for Scientific Research, Kolkata Centre, Kolkata 700098, India. 7Department of Pure and Applied Physics, Guru Ghasidas Viswavidyalaya, Koni, Bilaspur 495009,India. 8Department of Physics, Indian Institute of Technology Bombay, Powai, Mumbai,400076, India. 9Department of Physics, Panjab University, Chandigarh, India. )

Investigation of the structure of atomic nuclei in the vicinity of Z=82 shell closure become important due to co-existance of single particle and collective excitations. Three high-j obitals viz. d5/2 , h11/2 and h9/2 lie near proton Fermi surface along with low-j s1/2 and d3/2 orbitals, resulting in number of K-isomers in this mass region.
The iridium isotopes (Z = 77) are located in the...