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NSR database version of May 10, 2024.

Search: Author = P.Nazarzadeh

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2016NA19      Phys.Rev. C 93, 064605 (2016)

P.Nazarzadeh, M.Mohebali

Effect of deformation on the calculated half-lives of cluster emission using a proximity potential

RADIOACTIVITY ^{114,115,116,117,118}Ba, ^{119,120,121,122,123,124}Ce, ^124,125Pr, ^222,223,224Ac, ^{222,223,224,225,226,227,228}Th, ^{224,225,226,227}Pa, ^225,226,227U, ^225,227Np(¹⁶O); ²²⁴Ac, ^{223,224,225,226,227}Th, ^{225,226,227,228}Pa, ²²⁷U, ²²⁷Np(¹⁷O); ²²³Ra, ^224,225,226Ac, ^{219,220,221,222,223,224,225,226,227,228,229}Th, ^226,227Pa, ^227,228U, ²²⁷Np(¹⁸O); ^{223,224,225,226,227,228}Ra, ^226,227,228Ac, ^{224,225,226,227,228,229,230,231}Th, ^228,229Pa, ^{226,227,228,229,230,231,232}U, ²³¹Np(²⁰O); ²²⁸Ra, ²²⁹Ac, ^{227,228,229,230,231,232,233}Th, ²³¹Pa, ²³¹U, ²³¹Np(²²O); ^227,228Th, ^{227,228,229,230}Pa, ^{220,221,222,223,224,225,226,227,228,229,230,231,232}U, ^231,233Np, ^232,233Pu(²²Ne); ^228,229Ac, ²³⁰Th, ^{227,228,229,230,231,232,233,234}Pa(²³F); ^{223,224,225,226,227,228,229,230,231,232}Th, ^229,230,231Pa, ^{223,224,225,226,227,228,229,230,231,232,233,234,235,236}U, ²³³Np, ^233,234Pu(²⁴Ne); ^233,235U(²⁵Ne); ²³²Th, ^234,236U(²⁶Ne); ^{223,224,225,226,227,228,229,230,231,232,233,234,235,236}U, ^234,235,236Np, ^{228,229,230,231,232,233,234,235,236,237,238,239}Pu, ^237,238Am, ²³⁸Cm(²⁸Mg); ^{232,233,234,235,236,237}U, ^{232,233,234,235,236,237,238,239}Np, ^{232,233,234,235,236,237,238,239,240}Pu, ^238,239Am, ²⁴⁰Cm(³⁰Mg); ²³⁸Pu(³²Si); ²⁴⁰Pu, ²⁴¹Am, ²⁴²Cm(³⁴Si); calculated half-lives for cluster emissions using the proximity potential Christensen-Winther potential CW76 and considering deformation of the parent and daughter nuclei. Comparison with available experimental data, and theoretical results of the liquid drop model (LDM), and results obtained by a universal form of the proximity potential for spherical cluster emission.

doi: 10.1103/PhysRevC.93.064605
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2013DA12      Eur.Phys.J. A 49, 113 (2013)

S.Davoodabadi, P.Nazarzadeh

Emission of charged particles from excited compound nuclei ^{90, 94, 98}Mo

NUCLEAR REACTIONS ¹²C(⁷⁸Kr, X), E=8.52 MeV/nucleon;¹²C(⁸²Kr, X), E=7.69 MeV/nucleon;¹²C(⁸⁶Kr, X), E=9.31 MeV/nucleon; calculated charged particle σ from DNS (double nuclear system) using proximity potential. Compared with data and other calculations.

doi: 10.1140/epja/i2013-13113-9
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2001BE27      Phys.Rev. C63, 064607 (2001)

A.N.Behkami, Z.Kargar, P.Nazarzadeh, M.N.Nasrabadi

Microscopic Study of Fission Fragment Angular Distributions

NUCLEAR REACTIONS ¹⁷⁴Yb(¹²C, F), E=95 MeV; ²³²Th(¹⁶O, F), E=140 MeV; ²⁰⁸Pb(¹⁹F, F), E=110, 190 MeV; ²⁰⁸Pb(²⁴Mg, F), E=140, 210 MeV; calculated fission fragment angular distributions. Statistical scission model, comparisons with data.

doi: 10.1103/PhysRevC.63.064607
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