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NSR database version of May 10, 2024.

Search: Author = E.Javadimanesh

Found 8 matches.

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2013HA05      Int.J.Mod.Phys. E22, 1350007 (2013)

H.Hassanabadi, E.Javadimanesh, S.Zarrinkamar

Alpha decay half-lives for Pt isotopes

RADIOACTIVITY ^{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}Pt(α); calculated T_1/2, nuclear radii. Comparison with experimental data.

doi: 10.1142/S0218301313500079
Citations: PlumX Metrics

2013HA09      Chin.Phys.C 37, 044101 (2013)

H.Hassanabadi, E.Javadimanesh, S.Zarrinkamar, H.Rahimov

An angle-dependent potential and alpha-decay half-lives of deformed nuclei for 67≤Z≤91

RADIOACTIVITY ^152,154Ho, ¹⁵⁶Lu, ^159,160Ta, ¹⁵³Tm, ¹⁵⁶Hf, ¹⁵⁸W, ^163,165Re, ^166,167,169Ir, ¹⁷²Pt, ^170,173,177Au, ¹⁷⁶Hg, ^177,179,181Tl, ¹⁸⁰Pb, ^{188,192,193,197,199,201}Po, ^198,200,202At, ^{195,197,199,201,203}Rn, ^{201,202,203,204,206}Fr, ^203,205,207Ra, ^206,208Ac, ¹⁷⁴Ir, ^183,185,187Pb, ^{186,191,193,194,195}Bi, ²¹⁶Ac(α); calculated T_1/2. Angle-dependent potential, comparison with available data.

doi: 10.1088/1674-1137/37/4/044101
Citations: PlumX Metrics

2013HA38      Int.J.Mod.Phys. E22, 1350080 (2013)

H.Hassanabadi, E.Javadimanesh

Analytic solution for the potential barriers in alpha-decay process for Po isotopes

RADIOACTIVITY ^{190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,210,212,213,214,215,216,218}Po(α); calculated T_1/2. Comparison with available data.

doi: 10.1142/S0218301313500808
Citations: PlumX Metrics

2013JA10      Int.J.Mod.Phys. E22, 1350051 (2013)

E.Javadimanesh, H.Hassanabadi

An analysis of ¹⁷⁸Pb to ²³⁸U isotopes with the universal and Yukawa proximity potentials

NUCLEAR STRUCTURE Z=82-92; calculated nuclear structure parameters, decay constant. Comparison with available data.

doi: 10.1142/S0218301313500511
Citations: PlumX Metrics

2013JA16      Chin.Phys.C 37, 114102 (2013)

E.Javadimanesh, H.Hassanabadi, A.A.Rajabi, H.Rahimov, S. Zarrinkamar

Investigation of deformed nuclei with a new potential combination

RADIOACTIVITY ^152,154Ho, ¹⁵⁶Lu, ^159,160Ta, ¹⁵³Tm, ¹⁵⁶Hf, ¹⁵⁸W, ^163,165Re, ^166,167,169Ir, ¹⁷²Pt, ^170,173,177Au, ¹⁷⁶Hg, ^173,179,181Tl, ¹⁸⁰Pb, ^{188,192,193,197,199,201}Po, ^198,200,202At, ^{195,197,199,201,203}Rn, ^{201,202,203,204,206}Fr, ^203,205,207Ra, ^206,208Ac, ²¹⁷Pa, ¹⁷⁴Ir, ^183,185,187Pb, ^{186,191,193,194,195}Bi, ²¹⁶Ac, ²¹⁴Rn, ^212,214,216Po, ^216,218,220Ra, ^218,222Th, ²²²U, ^250,252,254Fm, ²⁵⁶Rf(α); calculated T_1/2. Yukawa potential, comparison with experimental data.

doi: 10.1088/1674-1137/37/11/114102
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2012JA09      Int.J.Mod.Phys. E21, 1250027 (2012)

E.Javadimanesh, H.Hassanabadi, A.A.Rajabi, H.Rahimov, S.Zarrinkamar

Half-lives of bismuth deformed isotopes in multiple approximation basis

RADIOACTIVITY ^{187,189,191,193,195,197,199,200,201,202,203,204,205,206,207,208,209,211,212,213,214}Bi(α); analyzed available data; calculated T_1/2. Angle-dependent potentials.

doi: 10.1142/S0218301312500279
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2012JA14      Chin.Phys.C 36, 964 (2012)

E.Javadimanesh, H.Hassanabadi, A.A.Rajabi, H.Rahimov, S.Zarrinkamar

Half-life of bismuth isotopes predicted by the Coulomb and proximity potential model; a proposition for the spherical nuclei

RADIOACTIVITY ^{187,189,191,193,195,197,199,200,201,202,203,204,205,206,207,208,209,211,212,213,214}Bi(α); calculated T_1/2. Coulomb and proximity potential model, comparison with available data.

doi: 10.1088/1674-1137/36/10/008
Citations: PlumX Metrics

2012JA15      Int.J.Mod.Phys. E21, 1250094 (2012)

E.Javadimanesh, H.Hassanabadi, A.A.Rajabi, H.Rahimov, S.Zarrinkamar

Half-lives with Yukawa proximity potential for alpha-decay process

RADIOACTIVITY ¹⁵⁵Lu, ¹⁵¹Dy, ¹⁵²Ho, ¹⁵⁴Tm, ¹⁵⁵Yb, ¹⁵⁶Lu, ¹⁵⁷Hf, ¹⁵⁸Ta, ¹⁵⁹W, ¹⁶⁰Re, ¹⁵⁴Ho, ¹⁵⁵Er, ¹⁵⁶Tm, ¹⁶⁰Ta, ¹⁶²Re, ¹⁷⁷Tl, ¹⁷⁹Tl, ¹⁸¹Tl, ¹⁹¹Pb, ^{188,192,193,195,199,201,205,207}Po, ^{196,197,198,199,200,201,202,203,204,205,207,208,209}At, ^201,207Rn, ^{200,204,205,206,207,208}Fr, ^{254,256,258,260,262,264,266,268}Rf, ^{258,260,262,264,266,268,270,272}Sg, ^{264,266,268,270,272,274,276}Hs, ^{268,270,272,274,276,278,280}Ds, ^{278,280,282,284}Cn, ^286,288Fl, ^290,292Lv(α); calculated T_1/2; deduced hindrance factor parameter as a ratio of theoretical to experimental T_1/2. Comparison with available data.

doi: 10.1142/S0218301312500942
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