NSR Query Results

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NSR database version of May 21, 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 205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237Ac, 208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239Th, 211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241Pa, 214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243U, 219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245Np(α); calculated T1/2. 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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 191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219At(α); calculated Q-values, T1/2. 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 178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220Pb(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 187,189,191,193,195Ir; 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
Citations: PlumX Metrics

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 246,252,248,254,250,256,255,253Fm, 252,256No, 255,257Lr, 258,256,263Rf, 257,259,263,256Db, 260,262,259,271,261,269Sg, 267,264,272,266,274,270Bh, 264,266,270,273,265,267Hs, 275,274,276,268,278Mt, 270,271,281,267,273,277Ds, 279,272,280,278Rg, 281Cn, 283,285,284,278,282Nh, 286,288Fl, 290Mc, 290,292Lv, 293,294Ts, 294Og(α); analyzed available data; calculated T1/2; deduced influence of isospin and angular momentum on α-decay half-lives. Comparison with available data.

doi: 10.1016/j.nuclphysa.2018.10.091
Citations: PlumX Metrics

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 246,248,250,252,253,254,255,256Fm, 252,256No, 255,257Lr, 256,258,263Rf, 256,257,259,263Db, 259,260,261,262,269,271Sg, 264,266,267,270,272,274Bh, 264,265,266,267,270,273Hs, 268,274,275,276,278Mt, 267,270,271,273,277,281Ds, 272,278,279,280Rg, 281Cn, 278,282,283,284,285Nh, 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, 286,287,288,289Fl, 287,288Mc, 290,291,292,293Lv, 294Ts, 294Og(α); calculated T1/2. 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 178,180,182,184,186,188,190,192,194Pb, 210Pb, 188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra(α); calculated T1/2 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 186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219Po(α); calculated Q-values, T1/2. 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 118,120,122,124Xe; calculated energy levels, J, π of gs, quasi-γ and quasi-β bands, E2 transition rates normalized to B(E2, 4g to 2g) 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 T1/2 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 T1/2 using analytical formulas of Royer and Denisov-Khudenko formula; deduced new parameters for both formulas using fit of data for 356 isotopes. Calculated T1/2 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 234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 244,246,248,250,252Cf, 248,250,252,254Fm(α); calculated α-decay branching ratios for gs and excited states using WKB barrier penetration probability, Q, α-particle angular momentum, T1/2 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 118,120,122,124,126,128Xe; 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 180,182,184,186,188,190,192,194,210Pb, 190,192,194,196,198,200,202,208,210,212,214,216,218Po, 198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 210,212,214,216,218,220,222,224,226,228,230,232Th, 218,220,222,224,226,228,230,232,234U(α); calculated T1/2 using CPPM (Coulomb and Proximity Potential Model); deduced T1/2 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 187,189,191,193,195,209,211,212,213,214Bi(α); calculated Q-value, T1/2. 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 257,268,269,271Sg, 262,263,270,271,272,274Bh, 261,262,273,275Hs, 266,267,275,276,278Mt, 265,266,277,279,281Ds, 272,274,278,279,280,281,282Rg, 271,279,281,283,285Cn, 279,281,282,283,284,285,286Nh, 283,284,285,286,287,288,289Fl, 286,292,287,288,289,290Mc, 287,288,290,291,292,293Lv, 290,292,293,294Ts, 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 112,114,116,118Pd, 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 98,100,102,104Ru, 102,104,106,108,110,112,114,116Pd, 106,108,110,112,114,116,118,120Cd, 118,120,122,124,126,128,130,132,134Xe, 130,132,134,136,142Ba, 134,136,138Ce, 140,148Nd, 140,142Sm, 142,144,152Gd, 154Dy, 156Er, 186,188,190,192,194,196,198,200Pt; 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, 110,112,114,116Pd, 118,120,126,128Xe; 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, 120,122,124,126Xe, 132,134Ce, 148Nd, 152Sm, 184,186,188Pt; calculated energy spectra, B(E2) and energy ratios. Comparison with available data.

doi: 10.1142/S0218301317500549
Citations: PlumX Metrics

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 209,211,212,213,214Bi, 200,201,202,204,206,208,210,211,214,216,218Po, 202At, 220,223,224,226Ra, 224,226,228,230,232Th, 228,230,232,234,236,238U, 279,280Rg, 285Cn, 282Nh, 286,288Fl, 293Lv, 294Og(α); calculated T1/2. 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, 282,283,284,285Cn, 286,287,288,289Fl, 290,291,292,293Lv, 294Og(α); calculated T1/2. 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 166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184Pt, 186,188,190,192,194,196,198Pt(α); calculated T1/2. 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, 188,192,193,195,199,201,205,207Po, 196,197,198,199,200,201,202,203,204,205,207,208,209At, 201,207Rn, 200,204,205,206,207,208Fr(α); calculated T1/2 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 166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190Pt(α); calculated T1/2, 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, 188,192,193,197,199,201Po, 198,200,202At, 195,197,199,201,203Rn, 201,202,203,204,206Fr, 203,205,207Ra, 206,208Ac, 174Ir, 183,185,187Pb, 186,191,193,194,195Bi, 216Ac(α); calculated T1/2. 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 190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,210,212,213,214,215,216,218Po(α); calculated T1/2. 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, 188,192,193,197,199,201Po, 198,200,202At, 195,197,199,201,203Rn, 201,202,203,204,206Fr, 203,205,207Ra, 206,208Ac, 217Pa, 174Ir, 183,185,187Pb, 186,191,193,194,195Bi, 216Ac, 214Rn, 212,214,216Po, 216,218,220Ra, 218,222Th, 222U, 250,252,254Fm, 256Rf(α); calculated T1/2. 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 187,189,191,193,195,197,199,200,201,202,203,204,205,206,207,208,209,211,212,213,214Bi(α); analyzed available data; calculated T1/2. 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 187,189,191,193,195,197,199,200,201,202,203,204,205,206,207,208,209,211,212,213,214Bi(α); calculated T1/2. 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, 188,192,193,195,199,201,205,207Po, 196,197,198,199,200,201,202,203,204,205,207,208,209At, 201,207Rn, 200,204,205,206,207,208Fr, 254,256,258,260,262,264,266,268Rf, 258,260,262,264,266,268,270,272Sg, 264,266,268,270,272,274,276Hs, 268,270,272,274,276,278,280Ds, 278,280,282,284Cn, 286,288Fl, 290,292Lv(α); calculated T1/2; deduced hindrance factor parameter as a ratio of theoretical to experimental T1/2. 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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