NSR Query Results

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NSR database version of April 27, 2024.

Search: Author = H.Hassanabadi

Found 57 matches.

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2023SA51      Int.J.Mod.Phys. E32, 2350047 (2023)

K.P.Santhosh, D.T.Akrawy, T.A.Jose, Ali H.Ahmed, H.Hassanabadi, S.S.Hosseini, V.Zanganah, L.Sihver

A systematic study of α-decay half-lives for Ac, Th, Pa, U and Np isotopes with A = 205-245 using the modified generalized liquid drop model

RADIOACTIVITY ^{205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237}Ac, ^{208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239}Th, ^{211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241}Pa, ^{214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243}U, ^{219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245}Np(α); calculated T_1/2. Comparison with available data.

doi: 10.1142/S0218301323500477
Citations: PlumX Metrics

2021GU19      Eur.Phys.J. A 57, 192 (2021); Erratum Eur.Phys.J. A 57, 256 (2021)

A.Guvendi, S.Zare, H.Hassanabadi

Vector boson oscillator in the spiral dislocation spacetime

doi: 10.1140/epja/s10050-021-00514-8
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2021SO17      Nucl.Phys. A1013, 122224 (2021)

H.Sobhani, H.Hassanabadi, D.Bonatsos, L.Sihver

An analytical description of the parity-doublet structure in an odd-A nucleus

NUCLEAR STRUCTURE ¹⁵¹Pm; analyzed available data; calculated energylevels, J, π, B(E1).

doi: 10.1016/j.nuclphysa.2021.122224
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2020HO08      Int.J.Mod.Phys. E29, 2050008 (2020)

S.S.Hosseini, H.Hassanabadi, D.T.Akrawy, A.H.Ahmed

Theoretical studies on Alpha decay half-lives of Astatine isotopes

RADIOACTIVITY ^{191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219}At(α); calculated Q-values, T_1/2. Comparison with available data.

doi: 10.1142/S0218301320500081
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2020SA23      Phys.Rev. C 101, 064610 (2020)

K.P.Santhosh, D..Akrawy, H.Hassanabadi, Al.H.Ahmed, T.A.Jose

α-decay half-lives of lead isotopes within a modified generalized liquid drop model

RADIOACTIVITY ^{178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220}Pb(α); calculated half-lives using modified generalized liquid drop model (MGLDM) with Akrawy, Royer, AKRE, and modified RenB formulas, and experimental Q(α) values. Comparison with available experimental half-lives, and with predicted half-lives in Coulomb and proximity potential model.

doi: 10.1103/PhysRevC.101.064610
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2020SO04      Eur.Phys.J. A 56, 29 (2020)

H.Sobhani, H.Hassanabadi, D.Bonatsos, F.Pan, S.Cui, Z.Feng, J.P.Draayer

Analytical study of the γ-unstable Bohr Hamiltonian with quasi-exactly solvable decatic potential

doi: 10.1140/epja/s10050-020-00048-5
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2020SO17      Nucl.Phys. A1002, 121956 (2020)

H.Sobhani, H.Hassanabadi, D.Bonatsos, F.Pan, J.P.Draayer

γ-Unstable Bohr Hamiltonian with sextic potential for odd-A nuclei

NUCLEAR STRUCTURE ^{187,189,191,193,195}Ir; analyzed available data; calculated energy ratios, B(E2) using the collective model of the γ-unstable Bohr Hamiltonian with the quasi exactly solvable sextic potential.

doi: 10.1016/j.nuclphysa.2020.121956
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2020ZA03      Nucl.Phys. A997, 121714(2020)

V.Zanganah, D.T.Akrawy, H.Hassanabadi, S.S.Hosseini, S.Thakur

Calculation of α-decay and cluster half-lives for ^197-226Fr using temperature-dependent proximity potential model

doi: 10.1016/j.nuclphysa.2020.121714
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2019AK02      Nucl.Phys. A983, 310 (2019)

D.T.Akrawy, H.Hassanabadi, Y.Qian, K.P.Santhosh

Influence of nuclear isospin and angular momentum on α-decay half-lives

RADIOACTIVITY ^{246,252,248,254,250,256,255,253}Fm, ^252,256No, ^255,257Lr, ^258,256,263Rf, ^{257,259,263,256}Db, ^{260,262,259,271,261,269}Sg, ^{267,264,272,266,274,270}Bh, ^{264,266,270,273,265,267}Hs, ^{275,274,276,268,278}Mt, ^{270,271,281,267,273,277}Ds, ^{279,272,280,278}Rg, ²⁸¹Cn, ^{283,285,284,278,282}Nh, ^286,288Fl, ²⁹⁰Mc, ^290,292Lv, ^293,294Ts, ²⁹⁴Og(α); analyzed available data; calculated T_1/2; deduced influence of isospin and angular momentum on α-decay half-lives. Comparison with available data.

doi: 10.1016/j.nuclphysa.2018.10.091
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2019AK07      Phys.Rev. C 100, 034608 (2019)

D.T.Akrawy, K.P.Santhosh, H.Hassanabadi

α-decay half-lives of some superheavy nuclei within a modified generalized liquid drop model

RADIOACTIVITY ^{246,248,250,252,253,254,255,256}Fm, ^252,256No, ^255,257Lr, ^256,258,263Rf, ^{256,257,259,263}Db, ^{259,260,261,262,269,271}Sg, ^{264,266,267,270,272,274}Bh, ^{264,265,266,267,270,273}Hs, ^{268,274,275,276,278}Mt, ^{267,270,271,273,277,281}Ds, ^{272,278,279,280}Rg, ²⁸¹Cn, ^{278,282,283,284,285}Nh, ^286,288Fl, ²⁹⁰Mc, ^290,292Lv, ^293,294Ts, ²⁹⁴Og(α); calculated half-lives for α decay using modified generalized liquid drop model (MGLDM). Comparison with other theoretical models, and with available experimental values.

doi: 10.1103/PhysRevC.100.034608
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2019AK13      Int.J.Mod.Phys. E28, 1950075 (2019)

D.T.Akrawy, H.Hassanabadi, S.S.Hosseini, K.P.Santhosh

Systematic study of alpha decay half-lives using new universal decay law

RADIOACTIVITY ²⁷¹Sg, ²⁷²Bh, ²⁷⁵Hs, ^275,276Mt, ²⁷⁹Ds, ^279,280Rg, ^283,285Cn, ^283,284Nh, ^{286,287,288,289}Fl, ^287,288Mc, ^{290,291,292,293}Lv, ²⁹⁴Ts, ²⁹⁴Og(α); calculated T_1/2. Comparison with available data.

doi: 10.1142/s0218301319500757
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2019HO06      Int.J.Mod.Phys. E28, 1950017 (2019)

S.S.Hosseini, H.Hassanabadi, D.T.Akrawy

α-Decay half-lives of even-even nuclei of Pb, Po, Rn and Ra isotopes

RADIOACTIVITY ^{178,180,182,184,186,188,190,192,194}Pb, ²¹⁰Pb, ^{188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^{198,200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^{202,204,206,208,210,212,214,216,218,220,222,224,226}Ra(α); calculated T_1/2 using emi-empirical, one-parameter model based on tunneling through a potential barrier with the centrifugal and over-lapping effects.

doi: 10.1142/S0218301319500174
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2019HO11      Int.J.Mod.Phys. E28, 1950043 (2019)

S.S.Hosseini, H.Hassanabadi, D.T.Akrawy, S.Zarrinkamar

Alpha-decay half-lives of polonium isotopes in the mass range of 186-218

RADIOACTIVITY ^{186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219}Po(α); calculated Q-values, T_1/2. Comparison with available data.

doi: 10.1142/S0218301319500435
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2019SO02      Nucl.Phys. A983, 229 (2019)

H.Sobhani, H.Hassanabadi

Non-degenerate γ-unstable Bohr Hamiltonian considering Killingbeck potential

NUCLEAR STRUCTURE ^{118,120,122,124}Xe; calculated energy levels, J, π of gs, quasi-γ and quasi-β bands, E2 transition rates normalized to B(E2, 4_g to 2_g) using Bohr Hamiltonian; compared to data; deduced staggering in gamma band.

doi: 10.1016/j.nuclphysa.2018.11.015
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2019SO03      Nucl.Phys. A986, 223 (2019)

H.Sobhani, H.Hassanabadi

The controlled single particle: A new concept in odd-mass nuclei

NUCLEAR STRUCTURE ¹⁵⁵Tb; calculated levels, J, π using "controlled single particle" model, suitable for odd-mass nuclei. Compared to data.

doi: 10.1016/j.nuclphysa.2019.03.015
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2019SO13      Nucl.Phys. A989, 135 (2019)

H.Sobhani, H.Hassanabadi

Application of the controlled single particle concept in the γ-rigid Bohr Hamiltonian for γ = 30 degrees

NUCLEAR STRUCTURE ¹⁸⁹Ir; calculated E((11/2)⁺) / E((7/2)⁺) and E((9/2)⁺) / E((7/2)⁺) for the gs-like band, the first γ-like band and the second γ-like band using Controlled Single Particle (CSP) concept and B(E2) transition rates, ground-like quantum numbers of states; compared with data.

doi: 10.1016/j.nuclphysa.2019.05.015
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2019SO20      Nucl.Phys. A992, 121621 (2019)

H.Sobhani, H.Hassanabadi

CSP-Z(5 over 2J+1) Application of the controlled single particle concept for the prolate to oblate nuclear shape phase transition in odd-A nuclei

doi: 10.1016/j.nuclphysa.2019.121621
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2018AK03      Nucl.Phys. A971, 130 (2018)

D.T.Akrawy, H.Hassanabadi, S.S.Hosseini, K.P.Santhosh

Systematic study of α-decay half-lives using Royer and related formula

RADIOACTIVITY N=50-180(α); calculated T_1/2 for 356 isotopes (separately odd-odd, even-even, odd-even and even-odd nuclei) using different semiempirical formulae; deduced formulae parameters, Royer formula having the highest predictive power using comparison with the data.

doi: 10.1016/j.nuclphysa.2018.01.018
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2018AK04      Nucl.Phys. A975, 19 (2018)

D.T.Akrawy, H.Hassanabadi, S.S.Hosseini, K.P.Santhosh

Nuclear isospin effect on α-decay half-lives Original research article

RADIOACTIVITY Z=52-118(α); calculated T_1/2 using analytical formulas of Royer and Denisov-Khudenko formula; deduced new parameters for both formulas using fit of data for 356 isotopes. Calculated T_1/2 compared to data.

doi: 10.1016/j.nuclphysa.2018.04.001
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2018HA18      Nucl.Phys. A974, 72 (2018)

H.Hassanabadi, S.S.Hosseini

Branching ratios of a-decay to ground and excited states of Fm, Cf, Cm and Pu

RADIOACTIVITY ^{234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{244,246,248,250,252}Cf, ^{248,250,252,254}Fm(α); calculated α-decay branching ratios for gs and excited states using WKB barrier penetration probability, Q, α-particle angular momentum, T_1/2 using proximity potential; compared branching ratios to data; deduced agreement for 0⁺ to 0⁺, 2⁺, 4⁺, 6⁺, 8⁺ calculations with data.

doi: 10.1016/j.nuclphysa.2018.03.006
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2018HA25      Phys.Rev. C 98, 014312 (2018)

H.Hassanabadi, H.Sobhani

Elimination of degeneracy in the γ-unstable Bohr Hamiltonian in the presence of an extended sextic potential

NUCLEAR STRUCTURE ^{118,120,122,124,126,128}Xe; calculated levels, J, π, g.s., γ₁ and β₁ bands, level staggering in γ band, and B(E2) using γ-unstable Bohr Hamiltonian with extended sextic potential. Comparison with experimental data taken from the ENSDF database.

doi: 10.1103/PhysRevC.98.014312
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2018HA33      Can.J.Phys. 96, 1059 (2018)

H.Hassanabadi, H.Sobhani

Observation of ultra-fine structures in energy levels of prolate nuclei

doi: 10.1139/cjp-2017-0403
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2018HO01      Nucl.Phys. A970, 259 (2018)

S.S.Hosseini, H.Hassanabadi, S.Zarrinkamar

A comparative analysis of alpha-decay half-lives for even-even ¹⁷⁸Pb to ²³⁴U isotopes

RADIOACTIVITY ^{180,182,184,186,188,190,192,194,210}Pb, ^{190,192,194,196,198,200,202,208,210,212,214,216,218}Po, ^{198,200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^{202,204,206,208,210,212,214,216,218,220,222,224,226}Ra, ^{210,212,214,216,218,220,222,224,226,228,230,232}Th, ^{218,220,222,224,226,228,230,232,234}U(α); calculated T_1/2 using CPPM (Coulomb and Proximity Potential Model); deduced T_1/2 vs mass number. Compared with data and published calculations.

doi: 10.1016/j.nuclphysa.2017.11.014
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2018HO04      Int.J.Mod.Phys. E27, 1850022 (2018)

S.S.Hosseini, H.Hassanabadi

Theoretical approaches on the α-decay of spherical Bismuth isotopes

RADIOACTIVITY ^{187,189,191,193,195,209,211,212,213,214}Bi(α); calculated Q-value, T_1/2. Comparison with experimental data.

doi: 10.1142/S0218301318500222
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2018SA41      Phys.Rev. C 98, 024625 (2018)

K.P.Santhosh, C.Nithya, H.Hassanabadi, D.T.Akrawy

α-decay half-lives of superheavy nuclei from a modified generalized liquid-drop model

RADIOACTIVITY ^{257,268,269,271}Sg, ^{262,263,270,271,272,274}Bh, ^{261,262,273,275}Hs, ^{266,267,275,276,278}Mt, ^{265,266,277,279,281}Ds, ^{272,274,278,279,280,281,282}Rg, ^{271,279,281,283,285}Cn, ^{279,281,282,283,284,285,286}Nh, ^{283,284,285,286,287,288,289}Fl, ^{286,292,287,288,289,290}Mc, ^{287,288,290,291,292,293}Lv, ^{290,292,293,294}Ts, ^291,292,294Og(α); ^296,297119, ^295,300120, ^304,306121, ^301,306122, ^310,312123, ^307,312124, ^316,318125, ^313,320126, ^320,322127, ^319,320128, ^326,327129, ^324,325130, ^334,336131, ^331,332132, ^329,330133, ^333,334134(α); calculated half-lives using the generalized liquid-drop model (GLDM) with 1977 nuclear proximity potential proposed by Blocki et al. Comparison with available experimental values, and with half-lives using GLDM model of Royer et al.

doi: 10.1103/PhysRevC.98.024625
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2018SO05      Nucl.Phys. A973, 33 (2018)

H.Sobhani, H.Hassanabadi, W.S.Chung

Investigation of Bohr Hamiltonian in presence of Killingbeck potential using bi-confluent Heun functions

NUCLEAR STRUCTURE ^{112,114,116,118}Pd, ^114,116Cd, ¹¹⁸Ru, ^118,120Xe, ^122,124Ba, ¹⁵⁰Nd, ¹⁵²Sm; calculated levels, J, π, dimensionless free parameters for each isotope for the triaxial deformation (Pd, Cd, Ru, Xe) and for the rotational case (Ba, Nd, Sm), staggering in γ-band; B(E2) for gs, γ₁, β₁ bands. Compared to available data.

doi: 10.1016/j.nuclphysa.2018.02.007
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2017AL01      Nucl.Phys. A957, 439 (2017)

M.Alimohammadi, H.Hassanabadi

Alternative solution of the gamma-rigid Bohr Hamiltonian in minimal length formalism

doi: 10.1016/j.nuclphysa.2016.10.004
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2017AL07      Nucl.Phys. A960, 78 (2017)

M.Alimohammadi, H.Hassanabadi, S.Zare

Investigation of Bohr-Mottelson Hamiltonian in γ-rigid version with position dependent mass

NUCLEAR STRUCTURE ^{98,100,102,104}Ru, ^{102,104,106,108,110,112,114,116}Pd, ^{106,108,110,112,114,116,118,120}Cd, ^{118,120,122,124,126,128,130,132,134}Xe, ^{130,132,134,136,142}Ba, ^134,136,138Ce, ^140,148Nd, ^140,142Sm, ^142,144,152Gd, ¹⁵⁴Dy, ¹⁵⁶Er, ^{186,188,190,192,194,196,198,200}Pt; calculated energy levels, J, B(E2) using Bohr-Mottelson Hamiltonian in γ-rigid version with position dependent mass. Compared to available data.

doi: 10.1016/j.nuclphysa.2017.01.003
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2017AL26      Eur.Phys.J. A 53, 129 (2017)

M.Alimohammadi, H.Hassanabadi

Investigation of the spectroscopy properties of deformed nuclei by combining the X(3) and E(5) models

NUCLEAR STRUCTURE ^100,104Ru, ^{110,112,114,116}Pd, ^{118,120,126,128}Xe; calculated gs, first β-band, first γ-band energy, J, B(E2) using model composed of part related to special critical points E(5) (phase transition between spherical oscillator and γ-soft) and X(3) (γ-rigid version of X(5)). Compared to data.

doi: 10.1140/epja/i2017-12319-1
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2017AL28      Nucl.Phys. A966, 34 (2017)

M.Alimohammadi, H.Hassanabadi

Investigation of the hybrid model with the Killingbeck potential in a variational approach

NUCLEAR STRUCTURE ^104,108Ru, ^118,120Xe, ^132,148Ce, ¹⁵⁰Nd, ¹⁵⁴Sm, ¹⁵⁶Gd; calculated states, J, π, transition rates, B(E2) using hybrid collective model with β-dependent Killingbeck potential and γ-dependent oscillator potential. Compared with other calculations and with data.

doi: 10.1016/j.nuclphysa.2017.05.090
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2017AL32      Int.J.Mod.Phys. E26, 1750054 (2017)

M.Alimohammadi, H.Hassanabadi

The X(3) model for the modified Davidson potential in a variational approach

NUCLEAR STRUCTURE ¹⁰²Mo, ^104,106,108Ru, ^{120,122,124,126}Xe, ^132,134Ce, ¹⁴⁸Nd, ¹⁵²Sm, ^184,186,188Pt; calculated energy spectra, B(E2) and energy ratios. Comparison with available data.

doi: 10.1142/S0218301317500549
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2017AR17      Can.J.Phys. 95, 1086 (2017)

A.Armat, H.Hassanabadi

Study of ground state binding energies of the single Ξ and Λ hypernuclei by using numerical computation

NUCLEAR STRUCTURE ²⁸Al, ³²S, ⁴⁰Ca, ⁵¹V, ⁵³Cr, ⁶⁴Cu, ⁷³Ge, ⁷⁶As, ⁸¹Se, ⁸¹Kr, ⁸⁹Y, ⁹⁴Zr, ¹⁰⁴Rh, ¹³⁹La, ²⁰⁸Pb; calculated ground state binding for lambda hypernuclei. Comparison with experimental data.

doi: 10.1139/cjp-2017-0011
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2017HA20      Nucl.Phys. A966, 82 (2017)

H.Hassanabadi, H.Sobhani, A.N.Ikot

Investigation of energy and B(E2) transition rates for Bohr Hamiltonian with generalized Davidson potential

NUCLEAR STRUCTURE ^108,114Pd, ¹¹⁶Te, ^122,124Xe, ^130,132Ba, ^156,158,160Gd, ^158,166Dy, ¹⁶⁴Er, ¹⁹²Pt; calculated rotational bands (ground band, γ₁, β₁ band) state energy, J, π, transition rates B(E2) using Bohr Hamiltonian with both original and generalized Davidson potential.

doi: 10.1016/j.nuclphysa.2017.05.103
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2017HO09      Int.J.Mod.Phys. E26, 1750024 (2017)

S.S.Hosseini, H.Hassanabadi, S.Zarrinkamar

Alpha decay half-lives for heavy and super-heavy isotopes

RADIOACTIVITY ^{209,211,212,213,214}Bi, ^{200,201,202,204,206,208,210,211,214,216,218}Po, ²⁰²At, ^{220,223,224,226}Ra, ^{224,226,228,230,232}Th, ^{228,230,232,234,236,238}U, ^279,280Rg, ²⁸⁵Cn, ²⁸²Nh, ^286,288Fl, ²⁹³Lv, ²⁹⁴Og(α); calculated T_1/2. Comparison with available data.

doi: 10.1142/S0218301317500240
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2017HO11      Chin.Phys.C 41, 064101 (2017)

S.S.Hosseini, H.Hassanabadi

Theoretical approaches to alpha decay half-lives of super-heavy nuclei

RADIOACTIVITY ²⁶⁷Rf, ²⁷¹Sg, ²⁷⁵Hs, ^279,281Ds, ^{282,283,284,285}Cn, ^{286,287,288,289}Fl, ^{290,291,292,293}Lv, ²⁹⁴Og(α); calculated T_1/2. Comparison with experimental data.

doi: 10.1088/1674-1137/41/6/064101
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2017HO23      Int.J.Mod.Phys. E26, 1750069 (2017)

S.S.Hosseini, H.Hassanabadi, H.Sobhani

Estimation of the alpha decay of Platinum isotopes using different versions of theoretical formula

RADIOACTIVITY ^{166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184}Pt, ^{186,188,190,192,194,196,198}Pt(α); calculated T_1/2. Comparison with experimental data.

doi: 10.1142/S0218301317500690
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2017IK01      Nucl.Phys. A963, 1 (2017)

A.N.Ikot, H.Sobhani, H.Hassanabadi

Study of energy and B(E2) transition rates for Davydov-Chaban Hamiltonian with generalized Davidson potential

NUCLEAR STRUCTURE ^112,114,116Pd, ^192,194,196Pt; calculated levels, J, π, rotational bands, B(E2) using Davydov-Chaban Hamiltonian with Davidson and generalized Davidson potential and assuming triaxial shape. Compared with data.

doi: 10.1016/j.nuclphysa.2017.03.010
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2017NA13      Eur.Phys.J.Plus 132, 171 (2017)

L.Naderi, H.Hassanabadi

Bohr Hamiltonian with hyperbolic Poschl-Teller potential for triaxial nuclei

NUCLEAR STRUCTURE ^98,100,102Ru; calculated energy spectra, B(E2). Comparison with available data.

doi: 10.1140/epjp/i2017-11445-5
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2017RA19      Eur.Phys.J. A 53, 187 (2017)

S.Rahmani, H.Hassanabadi

Decay properties of charm and bottom mesons in a quantum isotonic nonlinear oscillator potential model

doi: 10.1140/epja/i2017-12374-6
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2017SO01      Nucl.Phys. A957, 177 (2017)

H.Sobhani, H.Hassanabadi

Electric quadrupole transitions for some isotopes of Xenon; considering rigidity for γ = 30 degrees collective parameter

NUCLEAR STRUCTURE ^128,130,132Xe; calculated levels, B(E2) using Davydov-Chaban Hamiltonian with Davidson potential. Compared with available data.

doi: 10.1016/j.nuclphysa.2016.08.009
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2016AR04      Can.J.Phys. 94, 365 (2016)

A.Armat, H.Hassanabadi

Mass chains of light hypernuclei and separation energies of mirror hypernuclei from BWMH mass formula

NUCLEAR STRUCTURE ^3,4H, ^9,11Be, ¹¹C, ¹⁵N, ^15,16O; calculated hypernuclei masses, neutron- and proton-separation energies.

doi: 10.1139/cjp-2015-0616
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2016HO23      Int.J.Mod.Phys. E25, 1650109 (2016)

S.S.Hosseini, H.Hassanabadi, S.Zarrinkamar

Optimal temperature for alpha-decay half-lives with Yukawa proximity potential

RADIOACTIVITY ¹⁵¹Dy, ¹⁵⁵Yb, ¹⁵⁷Hf, ¹⁵⁹W, ¹⁵⁵Er, ¹⁹¹Pb, ^155,156Lu, ¹⁵⁴Ho, ^154,156Tm, ^158,160Ta, ^160,162Re, ^177,179,181Tl, ^{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(α); calculated T_1/2 for excited states; deduced temperature. Comparison with available data.

doi: 10.1142/S0218301316501093
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2016NE01      Nucl.Phys. A945, 80 (2016)

H.Neyazi, A.A.Rajabi, H.Hassanabadi

Exactly separable Bohr Hamiltonian with the Killingbeck potential for triaxial nuclei

doi: 10.1016/j.nuclphysa.2015.08.007
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2016SA54      Eur.Phys.J. A 52, 346 (2016)

K.Saeedi, H.Hassanabadi, S.Zarrinkamar

Spin-zero DKP equation with two time-dependent interactions

doi: 10.1140/epja/i2016-16346-0
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2015DA09      Eur.Phys.J. A 51, 69 (2015)

M.Darroodi, H.Hassanabadi, N.Salehi

The modified Woods-Saxon potential in the Duffin-Kemmer-Petiau equation

doi: 10.1140/epja/i2015-15069-0
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2015SA33      Eur.Phys.J. A 51, 100 (2015)

N.Salehi, H.Hassanabadi

Scattering amplitude of the Duffin-Kemmer-Petiau equation for the Yukawa potential for J = 0

doi: 10.1140/epja/i2015-15100-6
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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
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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
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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
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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
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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
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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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2011HA57      Phys.Rev. C 84, 064003 (2011)

H.Hassanabadi, B.H.Yazarloo, S.Zarrinkamar, A.A.Rajabi

Duffin-Kemmer-Petiau equation under a scalar Coulomb interaction

doi: 10.1103/PhysRevC.84.064003
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2009HA23      Int.J.Mod.Phys. E18, 1497 (2009)

H.Hassanabadi, A.A.Rajabi, M.M.Shojaei

Hyperspherical approach to study the Schrodinger equation for an N-particle system

doi: 10.1142/S0218301309013658
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2009ZA04      Int.J.Mod.Phys. E18, 1781 (2009)

S.Zarrinkamar, H.Hassanabadi, A.A.Rajabi

Mass terms in CP-conserving Weinberg three-Higgs-doublet model

doi: 10.1142/S021830130901383X
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