Enter your keyword

2-s2.0-85055131180

[vc_empty_space][vc_empty_space]

Computational aspect of fermi distribution application on fission yield data calculation

Kurniadi R.a

a Nuclear Phsyics and Biophysics Research Group, Institut Teknologi Bandung, Bandung, Indonesia

[vc_row][vc_column][vc_row_inner][vc_column_inner][vc_separator css=”.vc_custom_1624529070653{padding-top: 30px !important;padding-bottom: 30px !important;}”][/vc_column_inner][/vc_row_inner][vc_row_inner layout=”boxed”][vc_column_inner width=”3/4″ css=”.vc_custom_1624695412187{border-right-width: 1px !important;border-right-color: #dddddd !important;border-right-style: solid !important;border-radius: 1px !important;}”][vc_empty_space][megatron_heading title=”Abstract” size=”size-sm” text_align=”text-left”][vc_column_text]© 2018 The AuthorIn fission toy model (FTM), point particle treats as nucleon. It is assumed that nucleons do not interact between them; nucleon distribution adopts Fermi distribution function. The sigma parameter σ is introduced as the surface thickness of the nucleus in the model. One random value of sigma represents one fission event. Rupture neck is approximated by using polynomial of n-th order, where n is the even number. The spheres and neck surfaces shape the droplet. Elongation, which is the distance value between two centers of mass is obtained by summing two distances from the center of distribution function and distribution function intersection point. By this method, the elongation parameter value connects nucleon distribution with neck rupture function. This work will show fission yield data results from fission toy model, which combines of Fermi distribution and polynomial neck function.[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Author keywords” size=”size-sm” text_align=”text-left”][vc_column_text][/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Indexed keywords” size=”size-sm” text_align=”text-left”][vc_column_text]Fermi distribution,Fission yield,FTM[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Funding details” size=”size-sm” text_align=”text-left”][vc_column_text]This research is fully supported by Penelitian Dasar Unggulan Perguruan Tinggi KemenRistekDikti 2017–2018.[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”DOI” size=”size-sm” text_align=”text-left”][vc_column_text]https://doi.org/10.1016/j.rinp.2018.09.057[/vc_column_text][/vc_column_inner][vc_column_inner width=”1/4″][vc_column_text]Widget Plumx[/vc_column_text][/vc_column_inner][/vc_row_inner][/vc_column][/vc_row][vc_row][vc_column][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][/vc_column][/vc_row]