Synthesis of 250–253No in 206Pb+48Ca reaction

The dynamical cluster-decay model (DCM) is used to calculate the fusion evaporation residue cross-sections σxn for x=1-4 neutron emissions in the fusion reaction 206Pb+48Ca➔ 254No* at various incident energies. Considering the multipole deformations up to hexadecapole deformations β4i and configura...

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Main Authors: Niyti, Gupta Raj K.
Format: Article
Language:English
Published: EDP Sciences 2014-03-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/20146603066
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spelling doaj-c51b53d9cfba47f88f365effde14592c2021-08-02T16:02:52ZengEDP SciencesEPJ Web of Conferences2100-014X2014-03-01660306610.1051/epjconf/20146603066epjconf_inpc2013_03066Synthesis of 250–253No in 206Pb+48Ca reactionNiyti 0Gupta Raj K.1Department of Physics, Kurukshetra UniversityDepartment of Physics, Panjab University The dynamical cluster-decay model (DCM) is used to calculate the fusion evaporation residue cross-sections σxn for x=1-4 neutron emissions in the fusion reaction 206Pb+48Ca➔ 254No* at various incident energies. Considering the multipole deformations up to hexadecapole deformations β4i and configurations with “compact” orientation angles θci (θc=20 for 206Pb), the model is shown to give a good description of the measured individual light-particle decay channels, within one parameter fitting, the neck-length ΔR. Considering 204,206,207,208Pb-based reactions, the dependence of 2n-emission yields on the isotopic composition of compound nucleus (CN) is also studied within the DCM. Of the four Pb-isotopes considered, at a fixed excitation energy E*~20 MeV, ΔR is largest for CN with mass number 256, followed by 255, 254 and smallest for 252, which means to suggest that neutrons emission occurs earliest for 256, then for 255, 254 and finally for 252, in complete agreement with experimental data where 256No* has the highest crosssection and 252No* the lowest with 255,254No* lying in between. This result arises due to the penetrability factor, and is related to double magicity of both target and projectile nuclei. http://dx.doi.org/10.1051/epjconf/20146603066
collection DOAJ
language English
format Article
sources DOAJ
author Niyti
Gupta Raj K.
spellingShingle Niyti
Gupta Raj K.
Synthesis of 250–253No in 206Pb+48Ca reaction
EPJ Web of Conferences
author_facet Niyti
Gupta Raj K.
author_sort Niyti
title Synthesis of 250–253No in 206Pb+48Ca reaction
title_short Synthesis of 250–253No in 206Pb+48Ca reaction
title_full Synthesis of 250–253No in 206Pb+48Ca reaction
title_fullStr Synthesis of 250–253No in 206Pb+48Ca reaction
title_full_unstemmed Synthesis of 250–253No in 206Pb+48Ca reaction
title_sort synthesis of 250–253no in 206pb+48ca reaction
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2014-03-01
description The dynamical cluster-decay model (DCM) is used to calculate the fusion evaporation residue cross-sections σxn for x=1-4 neutron emissions in the fusion reaction 206Pb+48Ca➔ 254No* at various incident energies. Considering the multipole deformations up to hexadecapole deformations β4i and configurations with “compact” orientation angles θci (θc=20 for 206Pb), the model is shown to give a good description of the measured individual light-particle decay channels, within one parameter fitting, the neck-length ΔR. Considering 204,206,207,208Pb-based reactions, the dependence of 2n-emission yields on the isotopic composition of compound nucleus (CN) is also studied within the DCM. Of the four Pb-isotopes considered, at a fixed excitation energy E*~20 MeV, ΔR is largest for CN with mass number 256, followed by 255, 254 and smallest for 252, which means to suggest that neutrons emission occurs earliest for 256, then for 255, 254 and finally for 252, in complete agreement with experimental data where 256No* has the highest crosssection and 252No* the lowest with 255,254No* lying in between. This result arises due to the penetrability factor, and is related to double magicity of both target and projectile nuclei.
url http://dx.doi.org/10.1051/epjconf/20146603066
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