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NSR database version of April 27, 2024.

Search: Author = S.P.Dange

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2024NA05      Nucl.Sci.Eng. 198, 771 (2024)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron–Induced Fission of ²³⁸Pu

NUCLEAR REACTIONS ²³⁸Pu(n, F), E ∼ 1.9 MeV; measured reaction products, Eγ, Iγ. ⁷⁸Ge, ^83,84Se, ^84,86Br, ^85,87,88,89Kr, ^89,90Rb, ^91,92,93,94Sr, ^{91,92,93,94,95}Y, ^95,97Zr, ^99,101Mo, ^{101,102,104,105}Tc, ^105,107,108Ru, ^105,109Rh, ^111,112,113Ag, ^115,117Cd, ^{123,125,127,128,129,130}Sn, ^{127,129,130,131}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135}I, ^135,137,138Xe, ^138,139,140Cs, ^{139,140,141,142}Ba, ¹⁴²La, ^{140,141,143,145,146}Ce, ¹⁴⁶Pr, ^{147,149,151,152}Nd, ^151,153Pm, ^{153,155,156,157}Sm; deduced cumulative and independent yields, nubar. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries. The reactor APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2023.2224274
Citations: PlumX Metrics

2024NA06      Appl.Radiat.Isot. 208, 111304 (2024)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Independent isomeric yield ratios of fission products in the epi-cadmium neutron induced fission of ²³³U

NUCLEAR REACTIONS ²³³U(n, F)¹²⁸Sb/¹³⁰Sb/¹³²Sb/¹³¹Te/¹³³Te/¹³⁴I/¹³⁶I/¹³⁵Xe/¹³⁸Cs, E ∼ 1.9 MeV; measured reaction products, Eγ, Iγ; deduced independent isomeric yield ratios (IR), root mean square fragment angular momenta. Comparison with available data. The reactor APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1016/j.apradiso.2024.111304
Citations: PlumX Metrics

2023NA10      Nucl.Sci.Eng. 197, 485 (2023)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Post-Neutron Mass Yield Distribution in the Thermal Neutron-Induced Fission of ²³⁵U

NUCLEAR REACTIONS ²³⁵U(n, F)⁷⁸As/⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁸Rb/⁸⁹Kr/⁸⁹Rb/⁹⁰Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Y/⁹⁵Y/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰¹Tc/¹⁰²Tc/¹⁰³Ru/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰⁵Ru/¹⁰⁷Ru/¹⁰⁸Ru/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹²⁹Sb/¹³⁰Sn/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Te/¹³³I/¹³⁴Te/¹³⁵I/¹³⁵Xe/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Nd/¹⁵¹Pm/¹⁵²Nd/¹⁵³Pm/¹⁵³Sm/¹⁵⁵Sm, E thermal; measured reaction products, Eγ, Iγ; deduced cumulative and independent yields. Comparison with available data. The reactors CIRUS and APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2022.2133947
Citations: PlumX Metrics

2023NA13      Nucl.Sci.Eng. 197, 1133 (2023)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Post-Neutron Mass Yield Distribution in the Thermal Neutron Induced Fission of ²³³U

NUCLEAR REACTIONS ²³³U(n, F), E thermal; measured reaction products, Eγ, Iγ. Z=77-155; deduced cumulative, independent fission yields, mass chain yields. Comparison with available data. Two different reactor facilities at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2022.2142433
Citations: PlumX Metrics

2023NA14      Appl.Radiat.Isot. 197, 110804 (2023)

H.Naik, R.J.Singh, S.P.Dange

Charge distribution of light mass fission products in the thermal neutron induced fission of ²³³U, ²³⁵U and ²³⁹Pu

NUCLEAR REACTIONS ^233,235U, ²³⁹Pu(n, F), E thermal; measured reaction products, Eγ, Iγ. ^77,78Ga, ^79,80,83,84Ge, ^81,83,84As, ^{83,84,85,87,88}Se, ^{86,87,88,89,90}Br, ^{86,87,88,89,90,91,92,93,94,95}Kr, ^89,91Rb, ^91,92,93,94Sr, ^95,99Y, ^97,99,102Zr, ^101,104,105Mo, ^{103,104,105,106}Tc, ^104,105Nb, ^{105,107,108,109}Ru, ¹¹²Pd; deduced fractional cumulative yields, charge distribution parameters. The reactor CIRUS at Bhabha Atomic Research Centre (BARC), India, the reactor APSARA at BARC, India.

doi: 10.1016/j.apradiso.2023.110804
Citations: PlumX Metrics

2023NA17      Nucl.Sci.Eng. 197, 1265 (2023)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²²⁹Th

NUCLEAR REACTIONS ²²⁹Th(n, F)⁷⁷Ge/⁷⁸Ge/⁸³Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁹Rb/⁹¹Sr/⁹²Sr/⁹³Sr/⁹³Y/⁹⁴Y/⁹⁵Y/⁹⁵Zr/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰³Ru/¹⁰⁵Ru/¹⁰⁷Rh/¹¹²Ag/¹¹³Ag/¹¹⁵Cd/¹¹⁷Cd/¹²⁷Sb/¹²⁸Sb/¹²⁹Sb/¹³¹I/¹³²Te/¹³³Te/¹³⁴Te/¹³³I/¹³⁴I/¹³⁵I/¹³⁸Xe/¹³⁸Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²La/¹⁴³Ce/¹⁴⁴Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Pm, E ∼ 0.5 eV; measured reaction products, Eγ, Iγ; deduced post-neutron mass yields, cumulative product yields. The Standard I and Standard II asymmetric modes of fission. The highly enriched uranium–fueled light water–moderated swimming pool reactor APSARA.

doi: 10.1080/00295639.2022.2150029
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2023NA18      Nucl.Sci.Eng. 197, 1279 (2023)

H.Naik, R.J.Singh, W.Jang, S.P.Dange

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²⁴⁵Cm

NUCLEAR REACTIONS ²⁴⁵Cm(n, F)⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁸⁹Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹³Sr/⁹³Y/⁹⁴Y/⁹⁵Y/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰²Tc/¹⁰³Ru/¹⁰⁵Rh/¹⁰⁷Ru/¹⁰⁷Rh/¹⁰⁸Ru/¹¹¹Ag/¹¹²Ag/¹¹³Ag/¹¹⁵Cd/¹¹⁷Cd/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹²⁹Sb/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Sb/¹³³Te/¹³³I/¹³⁴I/¹³⁴Te/¹³⁵I/¹³⁵Xe/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Pm/¹⁵³Pm/¹⁵³Sm/¹⁵⁶Sm/¹⁵⁷Eu/¹⁵⁸Eu/¹⁶¹Gd, E ∼ 0.5 eV; measured reaction products, Eγ, Iγ; deduced relative and absolute cumulative and mass chain yields, comparison of mass yield distributions was made between the epi-cadmium and thermal neutron–induced fission to examine the role of excitation energy on the nuclear structure effect and P/V ratio. The reactor APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2022.2153577
Citations: PlumX Metrics

2023NA29      Nucl.Sci.Eng. 197, 3110 (2023)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²⁴¹Pu

NUCLEAR REACTIONS ²⁴¹Pu(n, F)⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁸⁹Rb/⁹⁰Rb/⁹¹Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Sr/⁹⁴Y/⁹⁵Y/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰¹Tc/¹⁰²Tc/¹⁰³Ru/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰⁵Ru/¹⁰⁵Rh/¹⁰⁷Ru/¹⁰⁷Rh/¹⁰⁸Ru/¹⁰⁹Rh/¹¹¹Ag/¹¹²Ag/¹¹³Ag/¹¹⁵Cd/¹¹⁷Cd/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁷Sb/¹²⁸Sn/¹²⁹Sn/¹³⁰Sn/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Sb/¹³³Te/¹³³I/¹²⁴Te/¹³⁴I/¹³⁵I/¹³⁵Xe/¹³⁶I/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Cs/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Nd/¹⁵¹Pm/¹⁵²Nd/¹⁵³Pm/¹⁵³Sm/¹⁵⁵Sm/¹⁵⁶Sm/¹⁵⁷Eu, E ∼ 0.5 eV; measured reaction products, Eγ, Iγ; deduced cumulative yields. Comparison with ENDF/B-VIII.0, JEFF-3.3 evaluated libraries. The reactor APSARA at the Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2023.2190725
Citations: PlumX Metrics

2023NA31      Eur.Phys.J. A 59, 230 (2023)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Charge distribution studies in the epi-cadmium neutron induced fission of ²⁴⁵Cm

NUCLEAR REACTIONS ²⁴⁵Cm(n, F)⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁹¹Sr/⁹²Sr/⁹³Sr/⁹⁵Y/⁹⁷Zr/¹⁰⁵Tc/¹⁰⁷Ru/¹⁰⁸Ru/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹³⁰Sn/¹²⁹Sb/¹³⁰Sb/¹³¹Sb/¹³³Sb/¹³¹Te/¹³²Te/¹³³Te/¹³⁴Te/¹³⁴I/¹³⁵I/¹³⁶I/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴²Ba/¹⁴⁴La/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁸Ce, E ∼ 0.5 eV; measured reaction products, Eγ, Iγ; deduced fission yields, fractional cumulative yields (FCY) and charge distribution parameters, isotopic yield distribution. The reactor APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1140/epja/s10050-023-01136-y
Citations: PlumX Metrics

2022NA02      Appl.Radiat.Isot. 179, 109993 (2022)

H.Naik, S.P.Dange, R.J.Singh

Charge distribution of light mass fission products in the fast neutron induced fission of ²³⁷Np, ²⁴¹Am and ²⁴³Am

NUCLEAR REACTIONS ²³⁷Np(n, F)⁸⁴Se/⁸⁶Br/⁸⁷Br/⁸⁸Kr/⁸⁹Kr/⁹⁰Kr/⁹¹Sr/⁹³Sr/⁹⁴Sr/⁹⁵Y/⁹⁷Zr/¹⁰³Mo/¹⁰⁵Tc/¹⁰⁶Tc/¹⁰⁷Ru, ²⁴¹Am(n, F)⁸⁴Se/⁸⁶Br/⁸⁷Br/⁸⁸Kr/⁸⁹Kr/⁹⁰Kr/⁹¹Rb/⁹²Sr/⁹³Sr/⁹⁴Sr/⁹⁵Y/⁹⁷Zr/¹⁰³Mo/¹⁰⁵Tc/¹⁰⁶Tc/¹⁰⁸Ru, ²⁴³Am(n, F)⁸⁴Se/⁸⁶Br/⁸⁷Br/⁸⁸Kr/⁸⁹Kr/⁹²Sr/⁹³Sr/⁹⁴Sr/⁹⁵Y/⁹⁷Zr/¹⁰⁵Tc/¹⁰⁶Tc/¹⁰⁸Ru, E thermal; measured reaction products, Eγ, Iγ; deduced fractional cumulative yields, charge distribution parameters. Comparison with available data.

doi: 10.1016/j.apradiso.2021.109993
Citations: PlumX Metrics

2022NA04      Nucl.Sci.Eng. 196, 16 (2022)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²³⁷Np

NUCLEAR REACTIONS ²³⁷Np(n, F), E ∼ 0.5 eV; measured reaction products, Eγ, Iγ. ^78,81As, ⁸⁰Ge, ^83,84Se, ^84,86,87Br, ^{85,87,88,89,90}Kr, ^88,89,90Rb, ^91,92,93,94Sr, ^91,93,94,95Y, ^95,97Zr, ^99,101,103Mo, ^{102,103,104,105}Tc, ^{103,105,107,108}Ru, ^105,107,109Rh, ^111,112,113Ag, ^115,117Cd, ^{123,125,127,129,130}Sn, ^{127,129,130,131}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135}I, ^135,137,139Xe, ^138,139,140Cs, ^{139,140,141,142}Ba, ^{141,143,144,145,146,147}Ce, ¹⁴⁶Pr, ^{147,149,151,152}Nd, ^149,151,153Pm, ^153,155,156Sm, ^156,157Eu; deduced cumulative or independent fission yields, mass chain yields. Comparison with ENDF/B-VIII.0, available data.

doi: 10.1080/00295639.2021.1951078
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33169.

2022NA12      Appl.Radiat.Isot. 182, 110137 (2022)

H.Naik, S.P.Dange, R.J.Singh

Charge distribution of heavy mass fission products in the thermal neutron induced fission of ²³³U, ²³⁵U and ²³⁹Pu

NUCLEAR REACTIONS ^233,235U, ²³⁹Pu(n, F), E thermal; measured reaction products, Eγ, Iγ. ^{127,128,129,130,131,132}Sn, ^{129,130,131,132}Sb, ^{131,132,133,134,136,137}Te, ^{134,135,136,137,138,139,140}I, ^{136,137,138,139,140,141,142,143,144}Xe, ^{139,140,142,143}Cs, ^{140,141,142,143,144,145,146}Ba, ^144,145,147La, ^{146,147,148,149}Ce; deduced fractional cumulative yields (FCY), isobaric charge distribution. Comparison with available data, ENDF/B library.

doi: 10.1016/j.apradiso.2022.110137
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33172.

2022NA14      Nucl.Sci.Eng. 196, 433 (2022)

H.Naik, R.J.Singh, W.Jang, S.P.Dange

Post-Neutron Mass Yield Distribution in the Thermal Neutron Induced Fission of ²³²U

NUCLEAR REACTIONS ²³²U(n, F), E thermal; measured reaction products, Eγ, Iγ. ^72,73,74Ga, ^77,78Ge, ⁷⁸As, ⁸¹As, ^83,84Se, ⁸⁴Br, ^86,87Br, ⁸⁵Kr, ^87,88,89,90Kr, ^88,89,90,91Rb, ^91,92,93,94Sr, ^{91,92,93,94,95}Y, ⁹⁹Mo, ¹⁰¹Mo, ^{101,102,103,104,105,106}Tc, ⁹⁵Zr, ⁹⁷Zr, ¹⁰³Ru, ¹⁰⁵Rh, ¹⁰⁷Rh, ¹²³Sn, ¹²⁵Sn, ^{127,128,129,130}Sn, ^{128,129,130,131,132,133}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135,136}I, ¹³⁵Xe, ^137,138,139Xe, ^138,139,140Cs, ¹⁴¹Ce, ¹⁴³Ce, ^145,146Ce, ¹⁴⁸Ce, ¹⁴⁶Pr, ¹⁴⁷Nd, ¹⁴⁹Nd, ^151,152Nd, ¹⁵¹Pm, ¹⁵³Pm, ¹⁵³Sm, ^155,156Sm, ^157,158Eu; measured reaction products, Eγ, Iγ; deduced cumulative and independent yields of various fission products, mass yield distributions. Comparison with available data, EXFOR library. Off-line gamma-ray spectrometric technique. The highly enriched uranium-fueled light water-moderated swimming pool reactor APSARA.

doi: 10.1080/00295639.2021.1993425
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33173.

2022NA18      Nucl.Sci.Eng. 196, 694 (2022)

H.Naik, R.J.Singh, S.P.Dange, W.Jang

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²⁴³Am

NUCLEAR REACTIONS ²⁴³Am(n, F), E∼0.5 eV; measured reaction products, Eγ, Iγ. ^83,82Se, ^84,86,87Br, ^85,87,89Kr, ^89,90Rb, ^91,92,93,94Sr, ^{91,82,93,94,95}Y, ^95,97Zr, ^99,101Mo, ^{102,104,105,106}Tc, ^103,105,108Ru, ^105,107,109Rh, ^{111,112,113,116}Ag, ¹¹⁷Cd, ¹¹⁹In, ^{123,125,127,128,129,130}Sn, ^{127,128,129,130,131,132,133}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135,136}I, ^135,137,138Xe, ^138,138,140Cs, ^{139,140,141,142}Ba, ^142,144La, ^{141,143,145,146,148}Ce, ¹⁴⁶Pr, ^{147,149,151,152}Nd, ^151,153Pm, ^155,156Sm, ^157,158Eu; deduced mass yields, cumulative yields of fission products, the average number of neutrons. Two different reactor facilities in Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2021.2014753
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33174.

2022NA21      Nucl.Sci.Eng. 196, 824 (2022)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Post-Neutron Mass Yield Distribution in the Thermal Neutron-Induced Fission of ²³⁹Pu

NUCLEAR REACTIONS ²³⁹Pu(n, F), E thermal; measured reaction products, Eγ, Iγ. ^78,81As, ^79,80Ge, ^83,84Se, ^84,86,87Br, ^{85,87,88,89,90}Kr, ^88,89,90,91Rb, ^91,92,93,94Sr, ^91,92,93,94Y, ^95,97Zr, ^99,101Mo, ^{101,102,103,104,105,106}Tc, ^{105,107,108,109}Ru, ^105,109Rh, ^111,113,116Ag, ¹¹⁷Cd, ¹¹⁹In, ^{123,125,127,128,129,130}Sn, ^129,130,131Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135,136}I, ^{135,137,138,139}Xe, ^{139,140,141,142}Ba, ^142,144La, ^{141,143,145,146,147}Ce, ¹⁴⁶Pr, ^{147,149,151,152}Nd, ^151,153,154Pm, ^{153,155,156,157}Sm, ^158,159Eu; deduced cumulative or independent yields. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries. The reactors CIRUS and APSARA at Bhabha Atomic Research Centre (BARC), India.

doi: 10.1080/00295639.2021.2025298
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33178.

2022NA25      Nucl.Sci.Eng. 196, 982 (2022)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of ²⁴¹Am

NUCLEAR REACTIONS ²⁴¹Am(n, F), E ∼ 0.5 eV; measured reaction products, Eγ, Iγ. ⁸⁰Ge, ⁸¹As, ^83,84Se, ⁸⁴Br, ^86,87Br, ⁸⁵Kr, ^87,88,89,90Kr, ^89,90,91Rb, ^91,92Sr, ^91,92,93,94Y, ⁹⁵Zr, ⁹⁷Zr, ^99,101,103Mo, ¹⁰²Tc, ^104,105,106Tc, ^103,105Ru, ¹⁰⁸Ru, ^105,107,109Rh, ^111,113Ag, ¹¹⁶Ag, ^115,117Cd, ¹¹⁹In, ^{123,125,127,129}Sn, ¹³⁰Sn, ^{129,130,131,132,133}Sb, ^{131,132,133,134}Te, ^{131,132,133,134,135,136}I, ¹³⁵Xe, ^137,138,139Xe, ^138,139,140Cs, ^{139,140,141,142}Ba, ^142,144La, ^140,141Ce, ^{143,144,145,146}Ce, ¹⁴⁸Ce, ¹⁴⁶Pr, ^147,149Nd, ¹⁵¹Pm, ^153,154Pm, ¹⁵³Sm, ^155,156,157Sm, ^157,158Eu, ^159,161Gd; deduced cumulative, independent and chain yields. Comparison with evaluated data. Two reactor facilities of Bhabha Atomic Research Centre (BARC) in India.

doi: 10.1080/00295639.2022.2038529
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33179.

2021NA05      Eur.Phys.J. A 57, 112 (2021)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-neutron mass yield distribution in the epi-cadmium neutron induced fission of ²⁴⁰Pu

NUCLEAR REACTIONS ²⁴⁰Pu(n, F)⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁸⁹Rb/⁹⁰Rb/⁹¹Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Sr/⁹⁴Y/⁹⁵Y/⁹⁵Zr/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰³Mo/¹⁰²Tc/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰³Ru/¹⁰⁵Ru/¹⁰⁸Ru/¹⁰⁵Rh/¹⁰⁹Rh/¹¹¹Ag/¹¹²Ag/¹¹³Ag/¹¹⁵Cd/¹¹⁷Cd/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁸Sn/¹³⁰Sn/¹²⁷Sb/¹²⁹Sb/¹³⁰Sb/¹³¹Sb/¹³²Sb/¹³³Sb/¹³¹Te/¹³²Te/¹³³Te/¹³⁴Te/¹³¹I/¹³²I/¹³³I/¹³⁴I/¹³⁵I/¹³⁶I/¹³⁵Xe/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Cs/¹⁴⁰Cs/¹⁴¹Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ba/¹⁴²Ba/¹⁴²La/¹⁴⁴La/¹⁴¹Ce/¹⁴³Ce/¹⁴⁴Ce/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁷Ce/¹⁴⁸Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁵¹Nd/¹⁵¹Pm/¹⁵³Sm/¹⁵⁵Sm/¹⁵⁶Sm/¹⁵⁷Eu, E thermal; measured reaction products, Eγ, Iγ; deduced cumulative and independent fission yields. Comparison with experimental data, EXFOR and ENDF/B-VIII.0 libraries.

doi: 10.1140/epja/s10050-021-00377-z
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33155.

2021NA07      Appl.Radiat.Isot. 173, 109718 (2021)

H.Naik, R.J.Singh, S.P.Dange

Charge distribution of light mass fission products in the ²³²U(n_th, f), ²³⁸Pu(n_th, f) and ²⁴⁴Cm(SF) reactions

NUCLEAR REACTIONS ²³²U, ²³⁸Pu(n, F)⁸¹As/⁸³Se/⁸⁴Se/⁸⁶Br/⁸⁷Br/⁸⁸Kr/⁸⁹Kr/⁹⁰Kr/⁹¹Rb/⁹¹Sr/⁹³Sr/⁹⁴Sr/⁹⁵Y/⁹⁷Zr/¹⁰³Mo/¹⁰⁵Tc/¹⁰⁷Ru/¹⁰⁸Ru, E thermal; measured reaction products, Eγ, Iγ; deduced fractional cumulative yields of various light mass fission products, charge distribution parameters. Comparison with available data.

RADIOACTIVITY ²⁴⁴Cm(SF); measured decay products, Eγ, Iγ. ^91,92,94Sr, ⁹⁷Zr, ¹⁰¹Mo, ¹⁰⁵Tc, ^105,108Ru, ¹¹²Pd; deduced fractional cumulative yields of various light mass fission products, charge distribution parameters. Comparison with available data.

doi: 10.1016/j.apradiso.2021.109718
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33157.

2021NA09      Nucl.Sci.Eng. 195, 717 (2021)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-Neutron Mass Yield Distribution in the Spontaneous Fission of ²⁵²Cf

RADIOACTIVITY ²⁵²Cf(SF); measured decay products, Eγ, Iγ; deduced cumulative and independent yields of various fission products, mass yield distribution parameters.

doi: 10.1080/00295639.2020.1866389
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33158.

2021NA10      Eur.Phys.J.Plus 136, 694 (2021)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-neutron mass chain yield distribution in the epi-cadmium neutron-induced fission of ²³²Th

NUCLEAR REACTIONS ²³²Th(n, F)⁷⁸As/⁸⁰Ge/⁸¹As/⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁶Br/⁸⁷Br/⁸⁷Kr/⁸⁸Kr/⁸⁹Kr/⁸⁹Rb/⁹⁰Kr/⁹⁰Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Sr/⁹⁴Y/⁹⁵Y/⁹⁵Zr/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰¹Tc/¹⁰²Tc/¹⁰³Mo/¹⁰³Tc/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰⁵Ru/¹⁰⁶Tc/¹⁰⁷Rh/¹⁰⁸Ru/¹⁰⁹Rh/¹¹²Ag/¹¹³Ag/¹¹⁶Ag/¹¹⁷Cd/¹¹⁹Cd/¹²³Sn/¹²⁵Sn/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹²⁹Sb/¹³⁰Sn/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Sb/¹³³Te/¹³³I/¹³⁴Te/¹³⁴I/¹³⁵I/¹³⁵Xe/¹³⁶I/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Xe/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Cs/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁴La/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Ce/¹⁴⁷Nd/¹⁴⁸Ce/¹⁴⁹Nd/¹⁵¹Nd/¹⁵²Nd/¹⁵³Pm, E>0.5 eV; measured reaction products, Eγ, Iγ; deduced cumulative and independent fission yields. Comparison with ENDF/B-VIII.0 evaluations, available data.

doi: 10.1140/epjp/s13360-021-01690-8
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2021NA12      Eur.Phys.J. A 57, 176 (2021)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Mass yield distribution in the fission of ²⁴⁴Cm induced by a spectrum of epi-cadmium to fast neutron

NUCLEAR REACTIONS ²⁴⁴Cm(n, F), E>0.0253 eV; measured reaction products, Eγ, Iγ. ^83,84Se, ^84,86,87Br, ^{85,87,88,89,90}Kr, ^89,90,91Rb, ^91,92,93,94Sr, ^92,93,94,95Y, ^95,97Zr, ^99,101,103Mo, ^102,104,105Tc, ^103,105,108Ru, ^105,107,109Rh, ^{111,112,113,116}Ag, ^115,117Cd, ¹¹⁹In, ^{123,125,127,128,129,130}Sn, ^{127,129,130,131,132,133}Sb, ^{131,132,133,134,135,136}I, ^{131,132,133,134}Te, ^135,137,138Xe, ^138,139,140Cs, ^{139,140,141,142}Ba, ^{141,143,144,145,146,147,148}Ce, ^142,144La, ¹⁴⁶Pr, ^147,149,151Nd, ^151,153Pm, ^153,155,156Sm, ^157,158Eu; deduced mass chain yields of fission products. Comparison with ENDF/B-VIII.0 library.

doi: 10.1140/epja/s10050-021-00485-w
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33159.

2021NA15      Ann.Nucl.Energy 162, 108493 (2021)

H.Naik, S.P.Dange, R.J.Singh, W.Jang

Post-neutron mass yield distribution in the thermal neutron induced fission of ²³⁸Pu

NUCLEAR REACTIONS ²³⁸Pu(n, F)⁸³Se/⁸⁴Se/⁸⁴Br/⁸⁵Kr/⁸⁶Br/⁸⁷Br/⁸⁷Kr/⁸⁸Kr/⁸⁸Br/⁸⁸Rb/⁸⁹Kr/⁸⁹Rb/⁹⁰Kr/⁹⁰Rb/⁹¹Rb/⁹¹Sr/⁹¹Y/⁹²Sr/⁹²Y/⁹³Sr/⁹³Y/⁹⁴Sr/⁹⁴Y/⁹⁵Y/⁹⁵Zr/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰²Tc/¹⁰³Tc/¹⁰³Ru/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰⁵Ru/¹⁰⁷Ru/¹⁰⁷Rh/¹⁰⁸Ru/¹⁰⁹Rh/¹¹²Ag/¹²⁵Sn/¹²⁷Sn/¹²⁷Sb/¹²⁸Sn/¹²⁸Sb/¹²⁹Sn/¹²⁹Sb/¹³⁰Sn/¹³⁰Sb/¹³¹Sb/¹³¹Te/¹³¹I/¹³²Sb/¹³²Te/¹³²I/¹³³Sb/¹³³Te/¹³³I/¹³⁴Te/¹³⁴I/¹³⁵I/¹³⁵Xe/¹³⁶I/¹³⁷Xe/¹³⁸Xe/¹³⁸Cs/¹³⁹Xe/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Cs/¹⁴⁰Ba/¹⁴¹Ba/¹⁴¹Ce/¹⁴²Ba/¹⁴²La/¹⁴³Ce/¹⁴⁴La/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁸Ce/¹⁴⁹Nd/¹⁵¹Nd/¹⁵¹Pm/¹⁵³Sm/¹⁵⁵Sm, E thermal; measured reaction products, Eγ, Iγ; deduced cumulative and independent fission yields, chain yields. Comparison with JEFF-3.3 evaluations, experimental data.

doi: 10.1016/j.anucene.2021.108493
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33160.

2020NA07      Eur.Phys.J. A 56, 82 (2020)

H.Naik, R.J.Singh, S.P.Dange

Post-neutron mass chain yield distribution in the thermal neutron induced fission of ²²⁹Th

doi: 10.1140/epja/s10050-020-00080-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33139.

2020NA22      Eur.Phys.J. A 56, 186 (2020)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-neutron mass yield distribution in the thermal neutron induced fission of ²⁴¹Pu

NUCLEAR REACTIONS ²⁴¹Pu(n, f), E=thermal; measured cumulative yields, post-neutron mass yields of fission products with mass A=83-115, 125-157 using charge distribution correction, independent yields of fission products with mass A=83-115, 125-157; deduced full width and tenth maxima (FWTM) of light- and heavy-mass yields[ reaction compared with ²²⁹Th(n, f) data; deduced nuclear structure effect - mass yield distribution in neutron-induced fission are fine structurearound asymmetric with triple humps for light-Z actinides, asymmetric with double humps for medium actinides (they have the higher mass yield, compared to EXFOR compilation of fission yield data); deduced fission products T_1/2, γ-ray evaluated abundance; compared to EXFOR compilation of fission yield data; yields compared with present work and with more than 10 other fission yields.

doi: 10.1140/epja/s10050-020-00184-y
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33144.

2020NA32      Eur.Phys.J. A 56, 227 (2020)

H.Naik, S.P.Dange, W.Jang, R.J.Singh

Post-neutron mass yield distribution in the thermal neutron induced fission of ²⁴⁵Cm

NUCLEAR REACTIONS ²⁴⁵Cm(n, F), E thermal; measured fission products, Eγ, Iγ. ^83,84Se, ⁸⁴Br, ⁸⁵Kr, ^86,87Br, ^87,88,89,90Kr, ^{87,88,89,90,91}Rb, ^91,92,93,94Sr, ^{91,92,93,94,95}Y, ^91,92,93,94Sr, ^95,97Zr, ^100,101Mo, ¹⁰³Mo, ^{102,103,104,105,106}Tc, ¹⁰³Ru, ¹⁰⁵Ru, ^107,108,109Ru, ^105,107,109Rh, ^111,112,113Ag, ¹¹⁶Ag, ^115,117Cd, ¹¹⁹In, ^123,125,127Sn, ^128,129,130Sn, ^{128,129,130,131}Sb, ^{131,132,133,134,135,136}I, ^{131,132,133,134}Te, ¹³⁵Xe, ^137,138,139Xe, ^{138,139,140,141}Cs, ^{139,140,141,142}Ba, ^142,144La, ^{141,143,145,147}Ce, ¹⁴⁸Ce, ¹⁴⁶Pr, ^147,149Nd, ¹⁵²Nd, ¹⁵¹Pm, ^153,154Pm, ^{152,153,154,155,156,157}Sm, ^157,158,159Eu, ^161,162Gd; deduced cumulative, independent and chain yields. Comparison with ENDF/B-VIII.0 library.

doi: 10.1140/epja/s10050-020-00228-3
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33145.

2017NA17      Appl.Radiat.Isot. 127, 92 (2017)

H.Naik, R.J.Singh, S.P.Dange

Charge distribution of light mass fission products in the fast neutron induced fission of ²³²Th, ²³⁸U, ²⁴⁰Pu and ²⁴⁴Cm

NUCLEAR REACTIONS ²³²Th, ²³⁸U, ²⁴⁰Pu, ²⁴⁴Cm(n, F)⁸⁵Se/⁸⁶Se/⁸⁹Kr/⁹⁰Kr/⁹¹Kr/⁹¹Rb/⁹¹Sr/⁹²Kr/⁹²Rb/⁹²Sr/⁹³Kr/⁹³Rb/⁹³Sr/⁹⁴Sr/⁹⁵Y/⁹⁷Zr/¹⁰³Mo/¹⁰⁵Tc/¹⁰⁶Tc/¹⁰⁸Ru/¹¹²Pd, E fast; measured fission products; deduced fractional cumulative yields, charge distribution parameters. Comparison with available data.

doi: 10.1016/j.apradiso.2017.05.009
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33106.

2007NA01      Nucl.Phys. A781, 1 (2007)

H.Naik, S.P.Dange, A.V.R.Reddy

Charge distribution studies in the odd-Z fissioning systems

NUCLEAR REACTIONS ²³⁷Np, ^241,243Am(n, F), E=fast; measured fission fragment isotopic yields, charge distributions; deduced parameters, local odd-even effect, shell effect. Radiochemical and gamma ray spectrometric technique.

doi: 10.1016/j.nuclphysa.2006.10.082
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33026.

2007NA04      Eur.Phys.J. A 31, 195 (2007)

H.Naik, S.P.Dange, R.J.Singh, A.V.R.Reddy

Single-particle spin effect on fission fragment angular momentum

NUCLEAR REACTIONS ²⁴³Am(n, F)¹²⁸Sb/¹³⁰Sb/¹³²Sb/¹³¹Te/¹³³Te/¹³²I/¹³⁴I/¹³⁶I/¹³⁵Xe/¹³⁸Cs, E=fast; measured isomeric yield ratios; deduced fission fragment angular momenta, single-particle spin effect. Comparison with results from other fissioning systems.

doi: 10.1140/epja/i2006-10171-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33016.

2005DA34      J.Radioanal.Nucl.Chem. 266, 79 (2005)

T.Datta, S.P.Dange, H.Naik

Single nucleon transfer reactions near Coulomb barrier on ¹⁹⁷Au

NUCLEAR REACTIONS ¹⁹⁷Au(¹²C, ¹¹C), (¹²C, ¹³C), (¹⁶O, ¹⁵O), (¹⁶O, ¹⁷O), E ≈ 6-7 MeV/nucleon; measured yield ratios, high spin yield fraction; deduced reaction mechanism features. Radiochemical and off-line spectrometric techniques.

doi: 10.1007/s10967-005-0872-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6011.

2005NA05      Phys.Rev. C 71, 014304 (2005)

H.Naik, S.P.Dange, R.J.Singh

Angular momentum of fission fragments in low energy fission of actinides

NUCLEAR REACTIONS ²³²Th, ^232,238U, ^238,240Pu, ²⁴⁴Cm(n, F)¹²⁸Sb/¹³⁰Sb/¹³²Sb/¹³¹Te/¹³³Te/¹³²I/¹³⁴I/¹³⁶I/¹³⁵Xe/¹³⁸Cs, E=thermal, fast; measured isomer yield ratios; deduced fission fragment angular momenta. Spin-dependent statistical model analysis.

doi: 10.1103/PhysRevC.71.014304
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33011.

2003NA35      Phys.Lett. B 576, 260 (2003)

H.Naik, S.P.Dange

Role of nuclear structure on the tilting mode

NUCLEAR REACTIONS ²³⁸U(α, F)¹³¹Te/¹³²I, E=40 MeV; measured Eγ, Iγ, fission fragments spin vs fragment emission angle; deduced relative high-spin yields, structure effects.

doi: 10.1016/j.physletb.2003.10.025
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6104.

2000NA07      Eur.Phys.J. A 7, 377 (2000)

H.Naik, S.P.Dange, R.J.Singh

Fission Fragment Angular Momentum in ODD-Z Fissioning Systems

NUCLEAR REACTIONS ²³⁷Np, ²⁴¹Am(n, F)¹²⁸Sb/¹³⁰Sb/¹³²Sb/¹³¹Sb/¹³¹Te/¹³³Te/¹³²I/¹³⁴I/¹³⁶I/¹³⁵Xe/¹³⁸Cs, E=reactor spectrum; measured γ spectrum with and without chemical separation of fission fragments, isomeric yield ratios; deduced fission fragment angular momentum, temperature, kinetic energy, saddle point deformation. Comparison with other measurements.

doi: 10.1007/s100500050405
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33017.

1999NA10      Nucl.Phys. A648, 45 (1999)

H.Naik, S.P.Dange, R.J.Singh, S.K.Das, R.Guin

Some Important Aspects of Fragment Angular Momentum in Medium Energy Fission of ²³⁸U

NUCLEAR REACTIONS ²³⁸U(α, F)¹³¹Te/¹³³Te/¹³⁴I, E=25-44 MeV; measured isomeric yield ratios; deduced fission fragments angular momenta, entrance channel parameters.

doi: 10.1016/S0375-9474(98)00639-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6099.

1998NA43      Radiochim.Acta 83, 109 (1998)

H.Naik, S.P.Dange, R.J.Singh

Charge Distribution for Light Mass Fission Products in the Thermal Neutron Induced Fission of ²²⁹Th, ²⁴¹Pu, ²⁴⁵Cm and ²⁵²Cf(SF)

NUCLEAR REACTIONS ²²⁹Th, ²⁴¹Pu, ²⁴⁵Cm(n, F), E=thermal; measured fission fragments charge distributions, cumulative yields; deduced charge dispersion parameter, shell effects.

RADIOACTIVITY ²⁵²Cf(SF); measured fission fragments charge distributions, cumulative yields; deduced charge dispersion parameter, shell effects.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33031.

1997NA01      Nucl.Phys. A612, 143 (1997)

H.Naik, S.P.Dange, R.J.Singh, S.B.Manohar

Systematics of Charge Distribution Studies in Low-Energy Fission of Actinides

NUCLEAR REACTIONS, ICPND ²²⁹Th, ²⁴¹Pu, ²⁴⁵Cm(n, F), E=thermal; measured fission products fractional, cummulative, independent, elemental yields, charge distribution parameters. Radiochemical, γ-spectrometric techniques.

RADIOACTIVITY ²⁵²Cf(SF); measured fission products fractional cummulative, independent, elemental yields, charge distribution parameters. Radiochemical separation, γ-spectrometric techniques.

doi: 10.1016/S0375-9474(96)00326-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33028.

1995DA17      Phys.Rev. C51, 3104 (1995)

T.Datta, H.Naik, S.P.Dange

Emission Angle Dependence of Fission Fragment Spin: Effects of single particle spin and tilting mode

NUCLEAR REACTIONS, ICPND ²³⁷Np(α, F)¹³²I/^132mI, E=29 MeV; measured residual nucleus independent isomeric yields or high-spin fraction, isomer production ratio, following fission at various emission angles; deduced quantitative effects of collective, single particle spins on fission fragment spin.

doi: 10.1103/PhysRevC.51.3104
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1143.

1995DA18      Z.Phys. A351, 305 (1995)

T.Datta, S.P.Dange, H.Naik, S.B.Manohar

Mass Asymmetry Dependence of Angular Distribution in ²³⁷Np(α₂₉ and 44 MeV, f): Single particle effect

NUCLEAR REACTIONS ²³⁷Np(α, F), E=29, 44 MeV; measured fission fragment angular anisotropy vs mass asymmetry; deduced odd-nucleon spin contribution to tilting mode variance. Data on other nuclei analyzed.

NUCLEAR STRUCTURE ²⁰¹Tl, ²⁰⁸Bi, ^210,211Po, ²¹³At, ²³⁴Pa, ^{235,236,237,238,239,240}Np, ^{240,242,237,238,239}Pu, ²⁴¹Am, ^245,247Bk, ^234,236U, ^244,246Cm, ²⁴⁸Cf; analyzed fission data; deduced odd-nucleon spin contribution to tilting mode variance.

doi: 10.1007/BF01290913
Citations: PlumX Metrics

1995NA07      Nucl.Phys. A587, 273 (1995)

H.Naik, S.P.Dange, R.J.Singh, T.Datta

Systematics of Fragment Angular Momentum in Low-Energy Fission of Actinides

NUCLEAR REACTIONS ²²⁹Th, ^235,233U, ^239,241Pu, ²⁴⁵Cm(n, F), E=thermal; measured fission fragment independent isomeric yield ratio for Sb, Te, I, Xe, Cs isotopes. Radiochemical, γ-spectroscopic techniques.

RADIOACTIVITY ²⁵²Cf(SF); measured fission fragment independent isomeric yield ratio for Sb, Te, I, Xe, Cs isotopes. Radiochemical, γ-spectroscopic techniques.

doi: 10.1016/0375-9474(94)00821-4
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33018.

1993DA08      Phys.Rev. C48, 221 (1993)

T.Datta, S.P.Dange, H.Naik, S.B.Manohar

Angular Distribution in Alpha-Induced Fission of ²³²Th and ²³⁸U

NUCLEAR REACTIONS ²³²Th, ²³⁸U(α, F), E=39.1 MeV; ²³⁸U(α, F), E=29 MeV; measured fission fragment σ(θ); deduced multi-chance fission role.

doi: 10.1103/PhysRevC.48.221
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6162.

1993NA22      Radiochim.Acta 62, 1 (1993)

H.Naik, S.P.Dange, T.Datta

Charge Distribution in the Mass Region 128-134 in Low Energy Fission of Actinides

NUCLEAR REACTIONS, ICPND ^233,235U, ^239,241Pu, ²⁴⁵Cm(n, F)¹²⁸Sn/¹³¹Sb/¹³²Te/¹³⁴Te, E=thermal; measured fission cumulative yeilds of residuals; deduced charge distribution systematics. Direct γ-spectrometric, radiochemical techniques.

doi: 10.1524/ract.1993.62.12.1
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33030.

1992DA17      Phys.Rev. C46, 1445 (1992)

T.Datta, S.P.Dange, H.Naik, S.Prakash

Emission-Angle Dependence of Fission Fragment Spin

NUCLEAR REACTIONS, ICPND ²³⁸U(α, F)¹³²I/^132mI, E=40 MeV; measured residue isomeric yield ratio vs emission angle; deduced fission fragment average spin at specific mass asymmetry vs emission angle.

doi: 10.1103/PhysRevC.46.1445
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0995.

1992NA08      Z.Phys. A342, 95 (1992)

H.Naik, T.Datta, S.P.Dange, R.Guin, P.K.Pujari, S.M.Sahakundu, S.Prakash

Effect of Entrance Channel Parameters on Fission Fragment Angular Momentum in Medium Energy Fission

NUCLEAR REACTIONS, ICPND ²³⁸U(α, F)¹³²I/^132mI, E=25-44 MeV; measured isomeric fission fragment yield ratios; deduced fission fragment angular momentum, entrance channel role. Collective rotational degrees of freedom, thermal equilibration model. Comparison with other data.

doi: 10.1007/BF01294493
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6105.

1988DA09      Z.Phys. A330, 103 (1988)

T.Datta, S.P.Dange, S.M.Sahakundu, S.Prakash, M.V.Ramaniah

Influence of Collective Rotational Degrees of Freedom in Medium Energy Fission

NUCLEAR REACTIONS ²³²Th, ²³⁸U(α, F), E=40 MeV; measured fission fragment independent isomeric yield ratios. ^131,133Te deduced rms angular momenta.

1988NA14      Z.Phys. A331, 335 (1988)

H.Naik, T.Datta, S.P.Dange, P.K.Pujari, S.Prakash, M.V.Ramaniah

Correlations of Fission Fragment Angular Momentum with Collective and Intrinsic Degrees of Freedom

NUCLEAR REACTIONS ²³⁵U, ²³⁹Pu, ²⁴⁵Cm(n, F), E=thermal; measured ^134,132I, fragment isomeric yield ratios. ^134,132I deduced deformation parameter at scission point. Radiochemical techniques. Statistical model.

RADIOACTIVITY ²⁵²Cf(SF); measured ^134,132I, fragment isomeric yield ratios. ^134,132I deduced deformation parameter at scission point. Radiochemical techniques. Statistical model.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33019.

1986DA11      Z.Phys. A324, 81 (1986)

T.Datta, S.P.Dange, S.K.Das, S.Prakash, M.V.Ramaniah

Influence of Fission Fragment Nuclear Structure on Scission Configuration in ²⁵²Cf(S.F.)

RADIOACTIVITY ²⁵²Cf(SF); measured independent fission products ¹¹¹Pd, ^131,133Te, ¹³⁴I, ¹³⁸Cs isomeric yield ratios; deduced fragment angular momenta. ²⁵²Cf deduced scission configuration fragment structure dependence.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30976.

1986DA24      Radiochim.Acta 39, 127 (1986)

S.P.Dange, H.Naik, T.Datta, A.V.R.Reddy, Satya Prakash, M.V.Ramaniah

Dependence of the Angular Momenta of Fission Fragments on Their Nuclear Structure

NUCLEAR REACTIONS ^233,235U, ^239,241Pu(n, F)¹³⁴I/^134mI, E=thermal; measured residual nucleus independent isomeric yield ratios, fission fragment charge vs angular momentum; deduced structure effects. Chemical separation, γ-ray spectral analyses.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30920.

1986DA26      J.Radioanal.Nucl.Chem. 108, 269 (1986)

S.P.Dange, H.Naik, T.Datta, R.Guin, Satya Prakash, M.V.Ramaniah

Effect of Shell Closure Proximity on Fragment Angular Momenta In ²⁴¹Pu/n(th), f/

NUCLEAR REACTIONS ²⁴¹Pu(n, F)¹³¹Te/^131mTe/¹³³Te/^133mTe/¹³²I/^132mI, E=thermal; measured fission product isomer yield ratio, angular momentum. Recoil catcher technique.

doi: 10.1007/BF02165185
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33021.

1986NA20      Radiochim.Acta 40, 175 (1986)

H.Naik, S.P.Dange, T.Datta, Satya Prakash, M.V.Ramaniah

Determination of Fractional Cumulative Yields of ⁹¹Sr, ⁹²Sr and ¹³⁴Te in the Thermal Neutron Induced Fission of ²³³U and ²⁴¹Pu

NUCLEAR REACTIONS ²³³U, ²⁴¹Pu(n, F)⁹¹Sr/⁹²Sr/¹³⁴Te, E=thermal; measured residuals cumulative yields following fission, fragment isobaric charge distribution for A=91, 92, 134.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30766.

1983DA18      Phys.Rev. C28, 1206 (1983)

T.Datta, S.M.Sahakundu, S.P.Dange, N.Chakravarty, R.Guin, Satya Prakash

Dependence of Fragment Angular Momentum on Entrance Channel in ²³⁶U Fission

NUCLEAR REACTIONS, ICPND ²³²Th(α, F), E=30 MeV; measured independent ^{131,131m,133,133m}Te isomeric yield ratios. ²³⁶U deduced fission fragment angular momentum entrance channel dependence. Activation technique. Statistical model.

doi: 10.1103/PhysRevC.28.1206
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6154.

1982DA01      Phys.Rev. C25, 358 (1982)

T.Datta, S.P.Dange, A.G.C.Nair, S.Prakash, M.V.Ramaniah

Fission Fragment Angular Momentum: Ratios of independent yields of isomers of ⁹⁵Nb and ¹³²I in thermal-neutron-induced fission of ²³³U

NUCLEAR REACTIONS, Fission ²³³U(n, F), E=thermal; measured independent isomeric yield ratios for ⁹⁵Nb, ¹³²I; deduced fragment angular momentum, deformation effect, prompt neutron number. Statistical model.

doi: 10.1103/PhysRevC.25.358
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30910.

1980DA06      Phys.Rev. C21, 1411 (1980)

T.Datta, S.P.Dange, S.B.Manohar, A.G.C.Nair, S.Prakash, M.V.Ramaniah

Charge Distribution in the Thermal Neutron Fission of ²⁴⁵Cm: Fractional Cumulative Yields of ¹³⁵I and ¹⁴⁰Ba

NUCLEAR REACTIONS ²⁴⁵Cm(n, F), E=th; measured fractional cumulative yields for ¹³⁵I, ¹⁴⁰Ba; deduced odd-even shell effects.

doi: 10.1103/PhysRevC.21.1411
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33069.

1979RA31      J.Inorg.Nucl.Chem. 41, 1649 (1979)

A.Ramaswami, S.P.Dange, S.Prakash, M.V.Ramaniah

Mass Yield from Thermal Neutron Induced Fission of ²⁴⁵Cm

NUCLEAR REACTIONS ²⁴⁵Cm(n, F), E=thermal; measured production σ for ^89,91Sr, ^95,97Zr, ⁹⁹Mo, ¹⁰³Ru, ¹¹¹Ag, ¹¹⁵Cd, ^121,125Sn, ¹²⁷Sb, ¹³¹I, ¹³²Te, ^133,135Xe, ¹⁴⁰Ba, ^141,143Ce, ¹⁴⁷Nd. Radiochemical, γ-counting techniques.

doi: 10.1016/0022-1902(79)80100-1
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1977RA13      Phys.Rev. C16, 716 (1977)

A.Ramaswami, S.Prakash, S.B.Manohar, S.P.Dange, P.P.Venkatesan, M.V.Ramaniah

Kinetic-Energy Distributions in the Reactor Neutron Fission of ²³²U and Thermal Neutron Fission of ²⁴¹Pu and ²⁴⁵Cm

NUCLEAR REACTIONS ²³²U, ²⁴¹Pu, ²⁴⁵Cm(n, F), E=reactor spectrum; measured recoil ranges of fission products in Al, average total kinetic energies, kinetic energy deficits.

doi: 10.1103/PhysRevC.16.716
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31682.

1975DA05      Phys.Rev. C11, 1251 (1975)

S.P.Dange, A.Ramaswami, S.B.Manohar, S.Prakash, M.V.Ramaniah

Fragment Kinetic Energy Distribution in the Fission of ²³⁷Np by Reactor Neutrons

NUCLEAR REACTIONS ²³⁷Np(n, F), E=reactor; measured recoil ranges of fission products, σ(E(fragment mass)).

doi: 10.1103/PhysRevC.11.1251
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30307.

1972PR11      J.Inorg.Nucl.Chem. 34, 2685 (1972)

S.Prakash, S.B.Manohar, S.P.Dange, A.Ramaswami

Kinetic Energy Distribution in the Thermal Neutron Fission of ²³³U and ²³⁹Pu

NUCLEAR REACTIONS, Fission ²³³U, ²³⁹Pu(n, F), E=thermal; measured recoil ranges; deduced kinetic energy distribution, average kinetic energy.

doi: 10.1016/0022-1902(72)80571-2
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33081.