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Search: Author = D.Naderi

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2023RA20      Int.J.Mod.Phys. E32, 2350028 (2023)

Z.Rashidpour, D.Naderi

An empirical formula for the alpha decay half-lives

RADIOACTIVITY ^106,108Te, ¹¹²Xe, ¹¹⁴Ba, ¹⁴⁴Nd, ^146,148Sm, ^148,150,152Gd, ^150,152,154Dy, ^152,154Er, ^154,156,158Yb, ^{156,158,160,162}Hf, ¹⁷⁴Hf, ^{160,162,164,166}W, ¹⁸⁰W, ^{162,164,166,168,170,172,174}Os, ¹⁸⁶Os, ^{168,170,172,174,176,178,180}Pt, ^188,190Pt, ^{174,176,178,180,182,184,186,188}Hg, ^{186,188,190,192,194}Pb, ²¹⁰Pb, ^{190,192,194,196,198,200,202,204,206}Po, ^{210,212,214,216,218}Po, ¹⁹⁸Rn, ^{204,206,208,210,212,214,216,218,220,222}Rn, ^204,206Ra, ^{210,212,214,216,218,220,222,224,226}Ra, ^{216,218,220,222,224,226,228,230,232}Th, ^{226,228,230,232,234,236,238}U, ^{232,234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{240,242,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^252,254,256No, ^256,258Rf, ^260,262Sg, ^264,266Hs, ²⁷⁰Hs, ²⁷⁰Ds, ^286,288Fl, ^290,292Lv, ²⁹⁴Og, ^107,109Te, ¹¹³Xe, ¹⁴⁷Sm, ¹⁵¹Gd, ^151,153Dy, ^153,155Er, ^155,157Yb, ¹⁵⁷Hf, ¹⁵⁹W, ¹⁶³W, ^169,171,173Os, ^{171,173,175,177}Pt, ^181,183Pt, ^175,177Hg, ^{195,197,199,201,203,205,207,209,211,213,215}Po, ^{201,203,205,207,209,211,213,215,217,219,221}Rn, ^{205,207,209,211,213,215,217,219,221}Ra, ^{213,215,217,219,221,223,225,227}Th, ²¹⁹U, ²²⁵U, ²³⁵U, ²²⁷Pu, ²⁴¹Cm, ²⁴⁷Cm, ²⁵¹Cf, ²⁵³Fm, ²⁵⁷Fm, ²⁵⁵No, ²⁵³Rf, ^259,261Sg, ²⁷¹Sg, ^265,267Hs, ²⁷³Hs, ²⁶⁷Ds, ^271,273Ds, ²⁷⁷Ds, ²⁸¹Ds, ¹⁴⁵Pm, ¹⁴⁷Eu, ¹⁵¹Eu, ^149,151Tb, ^153,155Tm, ¹⁶³Re, ¹⁶⁹Ir, ^175,177Ir, ^181,183,185Au, ^177,179Tl, ¹⁹⁵Bi, ²¹³Bi, ²⁰⁹Bi, ^{197,199,201,203,205,207,209,211,213,215}At, ^{201,203,205,207,209,211,213,215,217,219,221}Fr, ^{209,211,213,215,217,219,221,223,225}Ac, ²¹³Pa, ^{217,219,221,223,225,227,229,231}Pa, ^235,237Np, ^239,241,243Am, ²⁴⁵Bk, ²⁴⁹Bk, ²⁴⁵Es, ²⁵¹Es, ^255,257Lr, ^257,259Db, ²⁶³Db, ²⁶⁷Bh, ²⁷⁵Mt, ²⁷⁹Rg, ^283,285Nh, ²⁹³Ts, ¹¹²Cs, ¹⁴⁸Eu, ^152,154Ho, ¹⁵⁶Tm, ¹⁶²Ta, ^160,162Re, ¹⁶⁶Ir, ¹⁷⁰Ir, ¹⁷⁰Au, ¹⁷⁴Au, ^212,214Bi, ^{196,198,200,202,204,206,208,210,212,214}At, ^{204,206,208,210,212,214,216,218,220}Fr, ^206,208Ac, ^{214,216,218,220,222,224,226}Ac, ²¹²Pa, ^226,228,230Pa, ²⁵²Es, ²⁵⁶Db, ^264,266Bh, ^270,272,274Bh, ²⁶⁸Mt, ^276,278Mt, ²⁷²Rg, ^278,280Rg, ²⁷⁸Nh, ²⁸⁴Nh, ²⁹⁰Mc, ²⁹⁴Ts(α); calculated T_1/2; deduced an empirical formula to calculate alpha decay half-lives based on Geiger-Nuttall law for even-even, even-odd, odd-even and odd-odd nuclei.

doi: 10.1142/S0218301323500283
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2023SH04      Nucl.Phys. A1031, 122606 (2023)

B.Sharifi, D.Naderi

Theoretical study of superheavy elements ^{294, 297}Og using different versions of proximity potential

NUCLEAR REACTIONS ²⁴⁸Cf(⁴⁶Ca, X)²⁹⁴Og, ²⁴⁹Cf(⁴⁸Ca, X)²⁹⁷Og, E<55 MeV; analyzed available data; calculated of evaporation residue σ using nine versions of proximity potential as Prox77, Prox88, BW91, Bass73, Bass77, Denisov, CW76, GP77 and Guo2013.

doi: 10.1016/j.nuclphysa.2023.122606
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2021NA23      Chin.Phys.C 45, 094105 (2021)

D.Naderi, B.Sharifi

The entrance channel effect on the synthesis of a superheavy element ²⁹⁶119

NUCLEAR REACTIONS ²⁵⁸Md(³⁸Ar, X), ²⁶⁰Md(³⁶Ar, X), ²⁵⁷Fm(³⁹K, X), ²⁵²Es(⁴⁴Ca, X), ²⁵³Es(⁴³Ca, X), ²⁵⁴Es(⁴²Ca, X), ²⁵⁰Cf(⁴⁶Sc, X), ²⁵¹Cf(⁴⁵Sc, X), ²⁴⁷Bk(⁴⁹Ti, X), ²⁴⁸Bk(⁴⁸Ti, X), ²⁴⁹Bk(⁴⁷Ti, X), ²⁴⁵Cm(⁵¹V, X), ²⁴⁶Cm(⁵⁰V, X), ²⁴²Am(⁵⁴Cr, X), ²⁴³Am(⁵³Cr, X), ²⁴¹Pu(⁵⁵Mn, X), ²⁴²Pu(⁵⁴Mn, X), ²⁴⁴Pu(⁵²Mn, X), ²³⁶Np(⁶⁰Fe, X), ²³⁷Np(⁵⁹Fe, X), ²³⁸Np(⁵⁸Fe, X), ²³⁹Np(⁵⁷Fe, X), ²³⁶U(⁶⁰Co, X), ²³⁷U(⁵⁹Co, X), ²³²Pa(⁶⁴Ni, X), ²³³Pa(⁶³Ni, X), ²³¹Th(⁶⁵Cu, X), ²²⁶Ac(⁷⁰Zn, X), ²²⁵Ra(⁷¹Ga, X)²⁹⁶119, E<60 MeV; calculated evaporation residue σ; deduced role of asymmetry and mean fissility parameters in the synthesis of the superheavy element.

doi: 10.1088/1674-1137/ac0ee3
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2019NA30      Int.J.Mod.Phys. E28, 1950077 (2019)

D.Naderi, S.A.Alavi, V.Dehghani

Mass-split dependence of pre-scission neutron multiplicity by four-dimensional Langevin dynamics in ^{16, 18}O, ⁴⁰Ar and ⁶⁴Ni-induced fusion-fission reactions

NUCLEAR REACTIONS ¹⁴⁴Sm(¹⁸O, X), ¹⁹⁷Au(¹⁶O, X), ¹⁰⁹Ag(¹⁶O, X), ²³⁸U(⁴⁰Ar, X), E not given; analyzed available data; calculated fission dynamics using multidimensional Langevin model, including elongation, neck thickness, asymmetry parameter and orientation degree of freedom.

doi: 10.1142/s0218301319500770
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2019SA34      Z.Naturforsch. 74, 551 (2019)

M.Sayahi, V.Dehghani, D.Naderi, S.A.Alavi

Prediction of Alpha Decay Half-Lives of Z = 118-121 Superheavy Nuclei with A ≤ 300 by Using the Double-Folding Potential

NUCLEAR STRUCTURE Z=118-121; calculated α-decay T_1/2 using the density-dependent nuclear potential in the framework of the WKB method.

doi: 10.1515/zna-2019-0008
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2019SH42      Nucl.Phys. A991, 121616 (2019)

B.Sharifi, D.Naderi

The effect of deformation and orientation of colliding nuclei on synthesis of superheavy elements

doi: 10.1016/j.nuclphysa.2019.121616
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2017NA02      Chin.Phys.C 41, 024104 (2017)

D.Naderi, M.Salimi

Investigation of fission fragments average spin based on four dimensional Langevin dynamical model

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁸O, F), ²³²Th(¹⁶O, F), (¹²C, F), E<120 MeV; calculated average fragment spin and multiplicity of gamma rays, potential energy surface for the compound nuclei, ratio of the collective spins for different emission angles.

doi: 10.1088/1674-1137/41/2/024104
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2017NA11      Int.J.Mod.Phys. E26, 1730013 (2017)

D.Naderi, A.Farmani

Investigation of the ¹⁶O+¹⁹⁴Pt reaction: One- and two-dimensional dynamical interpretation

NUCLEAR REACTIONS ¹⁹⁴Pt(¹⁶O, X), E(cm)=72.8, 74.6, 79.3, 83 MeV; calculated fission time of compound nucleus, pre-scission neutron multiplicity, fission cross-section and probability.

doi: 10.1142/S0218301317500136
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2017NA33      Phys.Atomic Nuclei 80, 1073 (2017)

D.Naderi, A.Moradian, M.Zargooshi

Investigation of Ternary Fission of ₉₈²⁵²Cf Using Three-Cluster and Unified Ternary Fission Models

RADIOACTIVITY ²⁵²Cf(SF); calculated driving potential for fission to three fragments, yields vs mass numbers using Three-Cluster and Unified Ternary Fission Models.

doi: 10.1134/S1063778817060138
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2016NA05      Int.J.Mod.Phys. E25, 1650005 (2016)

D.Naderi

Effect of entrance channel on dynamics of heavy ions collision

NUCLEAR REACTIONS ¹⁷⁰Er(³⁰Si, X), ¹⁸⁴W(¹⁶O, X), ¹⁸¹ta(¹⁹F, X)²⁰⁰Pb, E(cm)<150 MeV; calculated fusion σ. Dinuclear systems (DNS) and one-dimensional (1D) Langevin equations, comparison with available data.

doi: 10.1142/S0218301316500051
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2015NA07      Int.J.Mod.Phys. E24, 1550010 (2015)

D.Naderi, M.Zargoosh

Study of alpha-decay half-lives with deformed, oriented daughter nuclei

RADIOACTIVITY ^{105,106,107,108,109,110}Te, ^{108,109,110,111,112,113}I, ^{109,110,111,112,113}Xe, ^112,114Cs, ¹¹⁴Ba(α); calculated T_1/2. Comparison with experimental data.

doi: 10.1142/S021830131550010X
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2014NA27      Phys.Rev. C 90, 024614 (2014)

D.Naderi

Role of asymmetry parameter and dissipation coefficient of K coordinate in angular distribution of fission fragments

NUCLEAR REACTIONS ²³²Th(¹⁶O, F)²⁴⁸Cf*, E=120, 140, 160 MeV; ²³⁸U(¹⁶O, F)²⁵⁴Fm*, E=90, 130, 148 MeV; ²⁴⁸Cm(¹⁶O, F)²⁶⁴Rf*, E=110, 130, 148 MeV; calculated angular distribution of fission fragments, dissipation coefficient for K as a function of asymmetry parameter. Four-dimensional Langevin equations with a nonconstant dissipation coefficient of K coordinate for symmetry and asymmetry fission. Comparison with experimental data.

doi: 10.1103/PhysRevC.90.024614
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2013NA09      Phys.Rev. C 87, 054618 (2013)

D.Naderi, M.R.Pahlavani, S.A.Alavi

Anisotropy of the angular distribution of fission fragments in heavy-ion fusion-fission reactions: The influence of the level-density parameter and the neck thickness

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁶O, X), E=85-150 MeV; ²⁰⁹Bi(²⁰Ne, X), E=120-220 MeV; calculated neutron multiplicity, and anisotropy of angular distribution of fission fragments as function of incident beam energy. Heavy ion fusion-fission reactions. Effects of the level-density parameter based on liquid drop model and neck thickness. One- and two-dimensional Langevin dynamical approach. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.054618
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2013NA25      Int.J.Mod.Phys. E22, 1350065 (2013)

D.Naderi

Study of cluster radioactivity: The influence of deformation of the cluster and daughter nuclei on cluster decay half-lives

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224,226}Ra, ^223,225Ac(¹⁴C), ²²⁸Th(²⁰O), ²³⁰Th(²⁴Ne), ²³⁰U(²²Ne), ²³¹Pa(²³F), (²⁴Ne), ^233,234U(²⁴Ne), ²³⁴U(²⁶Ne), (²⁸Mg), ²³⁸Pu(³²Si), ²³⁶Pu(²⁸Mg), ²³⁸Pu(²⁸Mg), (³⁰Mg), ²⁴²Cm(³⁴Si); calculated Q-value, T_1/2. Wentzel-Kramers-Brillouin method.

doi: 10.1142/S0218301313500651
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2013NA33      J.Phys.(London) G40, 125103 (2013)

D.Naderi

A dynamical interpretation of fusion-fission reactions using four-dimensional Langevin equations

NUCLEAR REACTIONS ¹⁹²Os(¹⁸O, X), (¹⁸O, F), ¹⁶⁹Tm(¹⁹F, X), (¹⁹F, F), E<150 MeV; calculated reaction products, En, In; deduced neutron multiplicity, σ. Four-dimensional Langevin equations.

doi: 10.1088/0954-3899/40/12/125103
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2012NA24      Phys.Rev. C 86, 044609 (2012)

D.Naderi

Calculation of fission probability using one- and two-body dissipation in fusion-fission reactions

NUCLEAR REACTIONS ¹⁵⁹Tb, ¹⁶⁹Tm, ¹⁸¹Ta(¹⁹F, F), ¹⁹⁷Au(¹⁷O, F), E=80-130 MeV; calculated compound nucleus fission rate, fission probability. Langevin dynamical approach. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.044609
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2012PA30      Eur.Phys.J. A 48, 129 (2012)

M.R.Pahlavani, D.Naderi

Study of fusion cross-section in heavy-ion fusion-fission reactions at around fusion barrier energies using the Langevin dynamical approach

NUCLEAR REACTIONS ⁹⁶Zr(⁶⁴Ni, X), E(cm)=123-157 MeV;¹⁰⁰Mo(⁶⁴Ni, X), E(cm)=127-144 MeV;¹²⁴Sn(⁵⁸Ni, X), E(cm)=150-190 MeV;¹⁶⁸Er(³⁴S, X), E(cm)=114-127 MeV;²⁰⁸Pb(³²S, X), E(cm)=139-185 MeV;²⁰⁸Pb(⁵⁰Ti, X), E(cm)=183-204 MeV; calculated fusion σ using coupled Langevin equations with Monte Carlo simulation. Compared with data and CCFULL calculations.

doi: 10.1140/epja/i2012-12129-y
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2011PA04      Int.J.Mod.Phys. E20, 45 (2011)

M.R.Pahlavani, D.Naderi, s.M.Mirfathi

Dynamical study of anisotropy in angular distribution of fission fragments in ¹⁶O+¹⁸¹Ta and ¹⁶O+²⁰⁸Pb fusion-fission reactions

NUCLEAR REACTIONS ¹⁸¹Ta, ²⁰⁸Pb(¹⁶O, X), E<140 MeV; calculated pre-scission neutron multiplicity, fission fragment σ(θ). Langevin equation and transition state model.

doi: 10.1142/S0218301311017314
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2011PA06      Phys.Rev. C 83, 024602 (2011)

M.R.Pahlavani, D.Naderi

Influence of dynamical parameters on pre-scission particles and fission probability in heavy-ion collisions

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁶O, F), E=90-125 MeV; ¹⁸¹Ta(¹⁹F, F), E=90-140 MeV; calculated fission probabilities and pre-scission particle (proton, neutron and α-particle) multiplicities using a stochastic approach to fission dynamics based on one- and three-dimensional Langevin equations. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.024602
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