Zobrazeno 1 - 5
of 5
pro vyhledávání: '"Shabnam Mohsina"'
Autor:
Neeraj Kumar, Shashi Verma, Shabnam Mohsina, Jhilam Sadhukhan, K. Rojeeta Devi, A. Banerjee, N. Saneesh, M. Kumar, Ruchi Mahajan, Meenu Thakur, Gurpreet Kaur, Anjali Rani, Neelam, Abhishek Yadav, Kavita, Rakesh Kumar, Unnati, S. Mandal, Suresh Kumar, B.R. Behera, K.S. Golda, A. Jhingan, P. Sugathan
Publikováno v:
Physics Letters B, Vol 814, Iss , Pp 136062- (2021)
The pre- and post-scission neutron multiplicities are measured for the fission of 208Rn, populated with the reactions 30Si+178Hf and 48Ti+160Gd in the excitation energy range of 54.5 - 80.8 MeV. We found significant differences in the pre-scission ne
Externí odkaz:
https://doaj.org/article/eea09b8fe04a4603ab1c1bc28536481f
Autor:
A. Banerjee, Jhilam Sadhukhan, S. Verma, Anjali Rani, P. Sugathan, Akhil Jhingan, Abhishek Yadav, K. S. Golda, Kavita, Meenu Thakur, B. R. Behera, Suresh Kumar, Rajesh Kumar, Ruchi Mahajan, Unnati, Neeraj Kumar, M. S. A. Kumar, K. Rojeeta Devi, S. K. Mandal, Neelam, Gurpreet Kaur, N. Saneesh, Shabnam Mohsina
Publikováno v:
Repositório Institucional da USP (Biblioteca Digital da Produção Intelectual)
Universidade de São Paulo (USP)
instacron:USP
Physics Letters B, Vol 814, Iss, Pp 136062-(2021)
Universidade de São Paulo (USP)
instacron:USP
Physics Letters B, Vol 814, Iss, Pp 136062-(2021)
The pre- and post-scission neutron multiplicities are measured for the fission of 208Rn, populated with the reactions 30Si + 178 Hf and 48Ti + 160 Gd in the excitation energy range of 54.5 - 80.8 MeV. We found significant differences in the pre-sciss
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::d12f11f94de56bd6deb6176e8d746a39
Autor:
Jhilam Sadhukhan, Shabnam Mohsina
Publikováno v:
Proceedings of 13th International Conference on Nucleus-Nucleus Collisions.
Autor:
Jhilam Sadhukhan, Shabnam Mohsina
Publikováno v:
Physical Review C. 101
Publikováno v:
Physical Review C. 96
The light-particle emission probability from an excited compound nucleus depends explicitly on the time-evolution of the system as the available internal excitation energy and, consequently, the particle decay widths depend on the instantaneous defor