NSR Query Results


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NSR database version of May 10, 2024.

Search: Author = S.Bhoi

Found 3 matches.

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2018BH03      Int.J.Mod.Phys. E27, 1850048 (2018)

S.Bhoi, B.Sahu

Unearthing radial independence for prediction of alpha-decay half-lives

RADIOACTIVITY 106,108Te, 112,114Xe, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154Er, 154,156,158Yb, 156,158,160Hf, 158,160,162,166W, 162,166,168,170,174,176,178,182,184,190Os, 168,180,188Pt, 174,176,180,182,184,188Hg, 188,186,190,210Pb, 190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,206,208,210,212,218,220,222Rn, 204,206,208,210,212,214,220,222,224,226Ra, 210,216,218,222,224,226,228,230,232Th, 224,226,228,230,232,234,236,238U, 230,232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,256No, 256,258Rf, 260,262Sg, 264,266,270Hs, 270Ds, 286,288Fl, 290,292Lv, 294Og(α), 141Ho, 165Ir, 171Au, 109I, 157Ta, 161Re, 167Ir, 185Bi, 177Tl(p); calculated Q-values, T1/2. Comparison with available data.

doi: 10.1142/S0218301318500489
Citations: PlumX Metrics


2017SA62      Phys.Rev. C 96, 044602 (2017)

B.Sahu, S.Bhoi

Potential for α-induced nuclear scattering, reaction and decay, and a resonance-pole-decay model with exact explicit analytical solutions

NUCLEAR REACTIONS 208Pb(α, α), (α, X), E=16-22 MeV; calculated elastic differential σ(θ, E), reaction σ(E) from optical model. Comparison with experimental data.

RADIOACTIVITY 190,194,196,198,200,202,204,206,208,210,212,214,216,218Po(α); calculated α-decay half-lives using optical model and resonance pole of analytical S matrix, comparison with experimental values. 210Pb, 212,214,216,218Po, 214,216,218,220,222Rn, 216,218,220,222,224,226Ra, 216,218,220,222,224,226,228,230,232Th, 222,224,226,228,230,232,234,236,238U, 232,234,236,238,240,242,244Pu, 240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf(α); calculated α-decay half-lives from resonance pole of analytical S matrix, and compared with experimental values. 112I, 149,151Tb, 159,162Ta, 175Ir, 181Au, 191,193,195,212,213,214Bi, 210,212At, 210,212,214,220,221Fr, 214,216,223,224,225,226Ac, 214,225,228,229,230Pa, 235,237Np, 235,239,241,243Am, 245,249Bk, 245,252Es, 257Md(α); calculated α-decay half-lives from the poles of the S matrix of the optical model, and compared with experimental values.

doi: 10.1103/PhysRevC.96.044602
Citations: PlumX Metrics


2016SA16      Phys.Rev. C 93, 044301 (2016)

B.Sahu, S.Bhoi

Viola-Seaborg relation for α-decay half-lives: Update and microscopic determination of parameters

RADIOACTIVITY 106,108Te, 112Xe, 114Ba, 144Nd, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154Er, 154,156,158Yb, 156,158,160,162,174Hf, 160,162,164,166,180W, 162,166,168,170,172,174,186Os, 168,170,174,176,178,180,188,190Pt, 174,176,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210Pb, 190,192,194,196,198,200,202,204,206,210,212,214,216,218Po, 198,204,206,208,210,212,214,216,218,220,222Rn, 210,212,214,216,218,220,222,224,226Ra, 216,218,220,222,224,226,228,230,232Th, 226,228,230,232,234,236,238U, 232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 260,266Sg(α); calculated ground-state to ground-state (l=0) half-lives and compared with experimental values; deduced analytic closed formula, as possible replacement of empirical Viola-Seaborg rule.

RADIOACTIVITY 144,145Nd, 145,146,147,148Pm, 146,147,148,149,150Sm, 130,131,132,133,134,135,136,137,138,139,140,141,148,151Eu, 135,136,137,138,139,140,141,142,143,148,149,150,151,152,153Gd, 136,137,138,139,140,141,142,144,145,149,150,151,152,154Tb, 138,139,140,141,142,143,144,145,146,147,149,150,151,152,153,154,155,156Dy, 140,141,142,143,144,145,147,148,149,150,151,152,153,154,155,156,157Ho, 145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,164Er, 153,154,155,156,157,158,159,160,161,162,163,164,165Tm, 154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,170Yb, 155,156,157,158,159,160,161,162,163,164,165,167,168,169,170,171,172,173,174Lu, 156,157,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178Hf, 157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,179Ta, 158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181W, 160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,183,184,185,186Re, 162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189Os, 164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191Ir, 166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193Pt(α); calculated α-decay half-lives using analytical formula and parameters deduced in the present work. Comparison with available experimental results.

doi: 10.1103/PhysRevC.93.044301
Citations: PlumX Metrics


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