NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = R.J.Singh Found 52 matches. 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, 91,92,93,94,95Y, 95,97Zr, 99,101Mo, 101,102,104,105Tc, 105,107,108Ru, 105,109Rh, 111,112,113Ag, 115,117Cd, 123,125,127,128,129,130Sn, 127,129,130,131Sb, 131,132,133,134Te, 131,132,133,134,135I, 135,137,138Xe, 138,139,140Cs, 139,140,141,142Ba, 142La, 140,141,143,145,146Ce, 146Pr, 147,149,151,152Nd, 151,153Pm, 153,155,156,157Sm; 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
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
2023NA03 Nucl.Sci.Eng. 197, 25 (2023) Post-Neutron Fission Product Yield Distribution in the Spontaneous Fission of 244Cm RADIOACTIVITY 244Cm(SF); measured decay products, Eγ, Iγ. 85Kr, 87,88Kr, 88,89Rb, 91,92Sr, 91Y, 93,94Y, 95Zr, 97Zr, 99Mo, 101Mo, 101Tc, 104,105Tc, 103Ru, 105Ru, 108Ru, 105Rh, 109Rh, 111,112,113Ag, 115Cd, 127Sb, 129,130,131,132,133Sb, 128Sn, 131I, 133,134I, 131,132,133,134Te, 135Xe, 137,138Xe, 138,139Cs, 139,140,141,142Ba, 141Ce, 143,144Ce, 146Ce, 146Pr, 147,149,151Nd, 151Pm, 155,156Sm; deduced post-neutron fission product yield distributions, parameters. Comparison with available data.
doi: 10.1080/00295639.2022.2103345
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
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
2023NA14 Appl.Radiat.Isot. 197, 110804 (2023) 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, 83,84,85,87,88Se, 86,87,88,89,90Br, 86,87,88,89,90,91,92,93,94,95Kr, 89,91Rb, 91,92,93,94Sr, 95,99Y, 97,99,102Zr, 101,104,105Mo, 103,104,105,106Tc, 104,105Nb, 105,107,108,109Ru, 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
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
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
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
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
2022NA02 Appl.Radiat.Isot. 179, 109993 (2022) 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
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, 85,87,88,89,90Kr, 88,89,90Rb, 91,92,93,94Sr, 91,93,94,95Y, 95,97Zr, 99,101,103Mo, 102,103,104,105Tc, 103,105,107,108Ru, 105,107,109Rh, 111,112,113Ag, 115,117Cd, 123,125,127,129,130Sn, 127,129,130,131Sb, 131,132,133,134Te, 131,132,133,134,135I, 135,137,139Xe, 138,139,140Cs, 139,140,141,142Ba, 141,143,144,145,146,147Ce, 146Pr, 147,149,151,152Nd, 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
2022NA12 Appl.Radiat.Isot. 182, 110137 (2022) 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. 127,128,129,130,131,132Sn, 129,130,131,132Sb, 131,132,133,134,136,137Te, 134,135,136,137,138,139,140I, 136,137,138,139,140,141,142,143,144Xe, 139,140,142,143Cs, 140,141,142,143,144,145,146Ba, 144,145,147La, 146,147,148,149Ce; deduced fractional cumulative yields (FCY), isobaric charge distribution. Comparison with available data, ENDF/B library.
doi: 10.1016/j.apradiso.2022.110137
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, 91,92,93,94,95Y, 99Mo, 101Mo, 101,102,103,104,105,106Tc, 95Zr, 97Zr, 103Ru, 105Rh, 107Rh, 123Sn, 125Sn, 127,128,129,130Sn, 128,129,130,131,132,133Sb, 131,132,133,134Te, 131,132,133,134,135,136I, 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
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, 91,82,93,94,95Y, 95,97Zr, 99,101Mo, 102,104,105,106Tc, 103,105,108Ru, 105,107,109Rh, 111,112,113,116Ag, 117Cd, 119In, 123,125,127,128,129,130Sn, 127,128,129,130,131,132,133Sb, 131,132,133,134Te, 131,132,133,134,135,136I, 135,137,138Xe, 138,138,140Cs, 139,140,141,142Ba, 142,144La, 141,143,145,146,148Ce, 146Pr, 147,149,151,152Nd, 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
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, 85,87,88,89,90Kr, 88,89,90,91Rb, 91,92,93,94Sr, 91,92,93,94Y, 95,97Zr, 99,101Mo, 101,102,103,104,105,106Tc, 105,107,108,109Ru, 105,109Rh, 111,113,116Ag, 117Cd, 119In, 123,125,127,128,129,130Sn, 129,130,131Sb, 131,132,133,134Te, 131,132,133,134,135,136I, 135,137,138,139Xe, 139,140,141,142Ba, 142,144La, 141,143,145,146,147Ce, 146Pr, 147,149,151,152Nd, 151,153,154Pm, 153,155,156,157Sm, 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
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, 123,125,127,129Sn, 130Sn, 129,130,131,132,133Sb, 131,132,133,134Te, 131,132,133,134,135,136I, 135Xe, 137,138,139Xe, 138,139,140Cs, 139,140,141,142Ba, 142,144La, 140,141Ce, 143,144,145,146Ce, 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
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
2021NA07 Appl.Radiat.Isot. 173, 109718 (2021) Charge distribution of light mass fission products in the 232U(nth, f), 238Pu(nth, 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
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
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
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, 85,87,88,89,90Kr, 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, 111,112,113,116Ag, 115,117Cd, 119In, 123,125,127,128,129,130Sn, 127,129,130,131,132,133Sb, 131,132,133,134,135,136I, 131,132,133,134Te, 135,137,138Xe, 138,139,140Cs, 139,140,141,142Ba, 141,143,144,145,146,147,148Ce, 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
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
2020NA07 Eur.Phys.J. A 56, 82 (2020) Post-neutron mass chain yield distribution in the thermal neutron induced fission of 229Th
doi: 10.1140/epja/s10050-020-00080-5
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 T1/2, 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
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, 87,88,89,90,91Rb, 91,92,93,94Sr, 91,92,93,94,95Y, 91,92,93,94Sr, 95,97Zr, 100,101Mo, 103Mo, 102,103,104,105,106Tc, 103Ru, 105Ru, 107,108,109Ru, 105,107,109Rh, 111,112,113Ag, 116Ag, 115,117Cd, 119In, 123,125,127Sn, 128,129,130Sn, 128,129,130,131Sb, 131,132,133,134,135,136I, 131,132,133,134Te, 135Xe, 137,138,139Xe, 138,139,140,141Cs, 139,140,141,142Ba, 142,144La, 141,143,145,147Ce, 148Ce, 146Pr, 147,149Nd, 152Nd, 151Pm, 153,154Pm, 152,153,154,155,156,157Sm, 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
2017NA17 Appl.Radiat.Isot. 127, 92 (2017) 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
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
2005NA05 Phys.Rev. C 71, 014304 (2005) 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
2004NA01 J.Phys.(London) G30, 107 (2004) Charge distribution in low energy fission of actinides NUCLEAR REACTIONS 232U, 238Pu(n, F), E=thermal; measured fission fragment charge distributions; deduced parameters, nuclear structure effects. RADIOACTIVITY 244Cm(SF); measured fission fragment charge distributions; deduced parameters, nuclear structure effects.
doi: 10.1088/0954-3899/30/2/010
2004NA44 Radiochim.Acta 92, 1 (2004) Fission fragment angular momentum in the spontaneous fission of 244Cm RADIOACTIVITY 244Cm(SF); measured fission fragments isomeric yield ratios; deduced fragment angular momentum distributions.
doi: 10.1524/ract.92.1.1.25406
2003NA02 Eur.Phys.J. A 16, 495 (2003) Charge distribution studies in the fast-neutron-induced fission of 232Th, 238U, 240Pu and 244Cm NUCLEAR REACTIONS 232Th, 238U, 240Pu, 244Cm(n, F), E=fast; measured fission product isotopic yields; deduced charge distribution parameters, average neutron multiplicity, proton odd-even effect, nuclear structure effects. Radiochemical and ∓ray spectrometric techniques, comparison with previous results.
doi: 10.1140/epja/i2002-10122-9
2000IY01 Nucl.Sci.Eng. 135, 227 (2000) R.H.Iyer, H.Naik, A.K.Pandey, P.C.Kalsi, R.J.Singh, A.Ramaswami, A.G.C.Nair Measurement of Absolute Fission Yields in the Fast Neutron-Induced Fission of Actinides: 238U, 237Np, 238Pu, 240Pu, 243Am, and 244Cm by Track-Etch-cum-Gamma Spectrometry NUCLEAR REACTIONS 238U, 237Np, 238Pu, 240Pu, 243Am, 244Cm(n, F), E=reactor; measured absolute isotopic fission yields. Fine structure and shell effects in mass distributions discussed, comparison with compiled data, activation technique.
doi: 10.13182/NSE00-A2136
2000NA07 Eur.Phys.J. A 7, 377 (2000) 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
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
1999PA55 Radiochim.Acta 87, 1 (1999) A.K.Pandey, H.Naik, R.J.Singh, A.Ramaswami, P.C.Kalsi, A.G.C.Nair, R.H.Iyer Absolute Fission Yields in the Spontaneous Fission of 244Cm: A new approach using lexan catcher-cum gamma ray spectrometry RADIOACTIVITY 244Cm(SF); measured Eγ, Iγ, (fragment)γ-coin; deduced fission yields. Recoil catcher technique. Comparison with compiled data.
doi: 10.1524/ract.1999.87.12.1
1998NA43 Radiochim.Acta 83, 109 (1998) 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
1996NA28 Radiochim.Acta 75, 69 (1996) H.Naik, A.G.C.Nair, P.C.Kalsi, A.K.Pandey, R.J.Singh, A.Ramaswami, R.H.Iyer Absolute Fission Yields in the Fast Neutron Induced Fission of 99.9997 Atom % Pure 238U using Track Etch-Cum Gamma Spectrometric Technique NUCLEAR REACTIONS 238U(n, F), E=fast; measured fission products Eγ, Iγ; deduced cumulative yields vs mass number, structure effects. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31538. 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
1993CH44 Radiochim.Acta 61, 9 (1993) N.Chakravarty, S.S.Rattan, R.J.Singh, A.Ramaswami Decay Studies of 197Tl(2.84 H) and 197mHg(23.8 H) RADIOACTIVITY 197Tl(β+), (EC); 197mHg(IT) [from 197Tl decay]; 197Hg(EC) [from 197mHg decay]; measured Eγ, Iγ; deduced 197Hg decay log ft. 197Hg deduced transition relative Iγ, γ-multipolarity, isomer decay ICC, IT, EC branching fractions.
1992RA29 Radiochim.Acta 57, 7 (1992) S.S.Rattan, N.Chakravarty, A.Ramaswami, R.J.Singh Alpha Particle Induced Reactions of 209Bi at 55.7 and 58.6 MeV NUCLEAR REACTIONS, ICPND 209Bi(α, n), (α, 2n), (α, 3n), (α, 4n), (α, 5n), (α, 6n), E=55.7, 58.6 MeV; measured residuals production σ. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1300. 1991RA26 Radiochim.Acta 55, 169 (1991) S.S.Rattan, A.Ramaswami, R.J.Singh, S.Prakash Alpha Particle Induced Fission of 209Bi at 55.7 and 58.6 MeV NUCLEAR REACTIONS, ICPND 209Bi(α, F)97Zr/99Mo/101Mo/112Pd/117mCd, E=55.7, 58.6 MeV; measured fission fragment production σ vs mass, residues fractional cumulative yields. Gamma ray spectrometry. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6001. 1990RA30 Radiochim.Acta 51, 55 (1990) S.S.Rattan, A.Ramaswami, R.J.Singh, S.Prakash Alpha Particle Induced Reactions on 27Al at 55.2 and 58.2 MeV NUCLEAR REACTIONS, ICPND 27Al(α, X)7Be/22Na/24Na/27Mg/28Mg/28Al/29Al, E=55.2, 58.2 MeV; measured residue production σ. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6005. 1989CH46 Radiochim.Acta 48, 1 (1989) N.Chakravarty, R.J.Singh, S.S.Rattan, A.Ramaswami, S.M.Sahakundu, S.Prakash, S.K.Ghosh Excitation Functions for Multi-Nucleon Emission in Helium Ion Reactions with 197Au NUCLEAR REACTIONS, ICPND 197Au(α, 2n), (α, 3n), (α, 4n), (α, 3np), (α, n2α), (α, 3He), (α, nα), E=threshold-50 MeV; measured residual production σ(E).
doi: 10.1524/ract.1989.48.12.1
1988RA38 J.Radioanal.Nucl.Chem. 125, 85 (1988) A.Ramaswami, G.K.Gubbi, R.J.Singh, Satya Prakash Cumulative Yields of Short-Lived Isotopes of Barium in the Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured cumulative 139,141,142Ba yields.
doi: 10.1007/BF02041752
1987RA24 Radiochim.Acta 41, 9 (1987) A.Ramaswami, S.S.Rattan, N.Chakravarty, R.J.Singh, S.B.Manohar, Satya Prakash, M.V.Ramaniah Charge Distribution Study in the Neutron Induced Fission of 237Np: Fractional cumulative yield of 134Te, 135I, and 138Xe NUCLEAR REACTIONS 237Np(n, F)134Te/135I/138Xe, E=reactor spectrum; measured fission product fractional cumulative yields, charge distribution widths. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30765. 1986RA10 Radiochim.Acta 39, 61 (1986) S.S.Rattan, R.J.Singh, S.M.Sahakundu, S.Prakash, M.V.Ramaniah Alpha Particle Induced Reactions of 209Bi and 63,65Cu NUCLEAR REACTIONS, ICPND 209Bi(α, 5n), (α, 4n), (α, 3n), E=threshold-47 MeV; measured residual production σ(E). 27Al(α, xnyp)22Na/23Na/28Mg, E=46.8, 44.3 MeV; 63,65Cu(α, xnyp)57Co/58Co/61Cu/64Cu/65Zn/66Ga/67Ga, E=47 MeV; measured residual production σ(E). Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0353. 1985RA29 Radiochim.Acta 38, 69 (1985) Alpha Induced Fission of 209Bi NUCLEAR REACTIONS, ICPND 209Bi(α, F)85Kr/85mKr/91Sr/92Sr/95Zr/97Zr/99Mo/103Ru/104Tc/105Ru/112Pd/115Cd, E=49.1, 44.9 MeV; measured fission product production σ, fission fragment mass distribution. 27Al(α, 5n4p), (α, 3n4p), (α, 3p), E=49.6, 45.4 MeV; measured residual production σ. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0450. 1983RA01 Phys.Rev. C27, 327 (1983) S.S.Rattan, A.V.Reddy, V.S.Mallapurkar, R.J.Singh, S.Prakash, M.V.Ramaniah Determination of Gamma Ray Energies and Abundances of 229Th RADIOACTIVITY 229Th(α); measured Eγ, Iγ. 225Ra deduced levels. High resolution Ge detector, radiochemical techniques.
doi: 10.1103/PhysRevC.27.327
1983RA34 Radiochim.Acta 33, 189 (1983) S.S.Rattan, A.V.R.Reddy, R.J.Singh, Satya Prakash, M.V.Ramaniah Charge Distribution in the Thermal-Neutron-Induced Fission of 229Th NUCLEAR REACTIONS 229Th(n, F)135I/140Ba, E=thermal; measured fractional independent residual yields following fission; deduced fission fragment charge distribution. Growth and decay of 135Xe, 140La. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33007. 1982SI14 Radiochim.Acta 31, 69 (1982) R.J.Singh, S.S.Rattan, A.V.R.Reddy, C.R.Venkatasubramani, A.Ramaswami, S.Prakash, M.V.Ramaniah Mass Distribution in the Thermal Neutron Induced Fission of 229Th NUCLEAR REACTIONS 229Th(n, F), E=thermal; measured fission fragment yield vs mass. 230Th deduced predominant asymmetric fission. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33002. Back to query form |