NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Sobhani Found 16 matches. 2023SO17 Chin.J.Phys.(Taiwan) 85, 475 (2023) A comprehensive semi-empirical formula for the half-lives of beta-decaying nuclei NUCLEAR STRUCTURE Z=2-107; analyzed available data; deduced β-decay formula, T1/2. Comparison with experimental data.
doi: 10.1016/j.cjph.2022.10.011
2022MO27 Eur.Phys.J. A 58, 125 (2022) R.Mohamadi pour, H.Sobhani, H.A.Kermani Intense magnetic field by twisted neutrinos beam in supernovae
doi: 10.1140/epja/s10050-022-00776-w
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
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
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
2019SO02 Nucl.Phys. A983, 229 (2019) 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
2019SO03 Nucl.Phys. A986, 223 (2019) 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
2019SO13 Nucl.Phys. A989, 135 (2019) 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
2019SO20 Nucl.Phys. A992, 121621 (2019) 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
2018HA25 Phys.Rev. C 98, 014312 (2018) 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
2018HA33 Can.J.Phys. 96, 1059 (2018) Observation of ultra-fine structures in energy levels of prolate nuclei
doi: 10.1139/cjp-2017-0403
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
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
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
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
2017SO01 Nucl.Phys. A957, 177 (2017) 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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