NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = I.Inci Found 13 matches. 2020IN03 Nucl.Phys. A1001, 121901 (2020) γ-Unstable odd deformed nuclei with the Kratzer potential: Multi-j case
doi: 10.1016/j.nuclphysa.2020.121901
2019IN02 Nucl.Phys. A991, 121611 (2019) Investigation of γ-unstable odd-even nuclei in the Collective model framework with the Morse potential NUCLEAR STRUCTURE 129,131Te, 135Ba, 155,157,159Tb, 187,189,191,193,195Ir; calculated energy levels, J, π, configurations, electric quadrupole transition ratios assuming odd-mass nucleus considered as a coupling of single nucleon in J=3/2 sp orbit with γ-unstable even core and using the Collective model Hamiltonian with the Morse potential in two versions, assumed fixed interaction strength between the nucleon and the core or deformation-dependent interaction; compared with published data; deduced Morse potential to be suitable to describe odd-even nuclei with structure in the γ-unstable region. To get more precise results, one has to add a term to explain degeneracy seen in the spectrum.
doi: 10.1016/j.nuclphysa.2019.12161a
2018IN04 Int.J.Mod.Phys. E27, 1850085 (2018) Coupling of a J = 3/2 nucleon to an even-even core with Davidson potential NUCLEAR STRUCTURE 187,189,191,193,195Ir; calculated energy levels, J, π, B(E2). Comparison with available data.
doi: 10.1142/S0218301318500854
2016IN03 Int.J.Mod.Phys. E25, 1650068 (2016) Study of Yb isotopes with the coherent state formalism NUCLEAR STRUCTURE 164,166,168,170,172,174,176,178Yb; calculated deformation parameters, excitation energies. Coherent state approach and interacting boson model (IBM), comparison with experimental data.
doi: 10.1142/S0218301316500683
2014IN01 Nucl.Phys. A924, 74 (2014) Test of the coherent state approach in the axially deformed region NUCLEAR STRUCTURE 168,170,172,174,176,178,180Hf; calculated transitional nuclei states, J, deformation, bands, B(E2) using coherent state approach with IBM and parameters from ground-state energy function. Compared with data.
doi: 10.1016/j.nuclphysa.2014.01.009
2011IN03 Phys.Rev. C 84, 024309 (2011) I.Inci, D.Bonatsos, I.Boztosun Electric quadrupole transitions of the Bohr Hamiltonian with the Morse potential NUCLEAR STRUCTURE 98,100,102,104Ru, 102,104,106,108Pd, 108,110,112,114,116,118Cd, 118,120,124,128Xe, 130,132,134,142Ba, 148Nd, 152Gd, 154Dy, 192,194,196,198Pt, 154Sm, 156Gd, 158Gd, 158,160Dy, 162Dy, 164Dy, 156,162,164,166,168,170Er, 166,168,170,172,174,176Yb, 174,176,178Hf, 182,184,186W, 186,188Os, 230,232Th, 234,236,238U, 238Pu, 250Cf; calculated B(E2) ratios for ground-state bands and interband transitions in γ-soft and deformed nuclei. Asymptotic iteration method (AIM) for collective Bohr Hamiltonian with the Morse potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.024309
2010BO25 J.Phys.:Conf.Ser. 205, 012020 (2010) D.Bonatsos, I.Boztosun, I.Inci A long sought result: Closed analytical solutions of the Bohr Hamiltonian with the Morse potential 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, 140,148,150Nd, 140,142,152,154Sm, 142,144,152,154,156,158,160,162Gd, 158,160,162,164,166Dy, 156,160,162,164,166,168,170Er, 164,166,168,170,172,174,176,178Yb, 168,170,172,174,176,178,180Hf, 176,178,180,182,184,186W, 178,180,184,186,188Os, 186,188,190,192,194,196,198,200Pt, 228Ra, 228,230,232Th, 232,234,236,238U, 238,240,242,248Cm, 250Cf; calculated low-lying 0+, 2+, 4+ states, β and γ bandheads, deformation using Bohr Hamiltonian with Morse potential; deduced Morse potential shapes. Compared with data.
doi: 10.1088/1742-6596/205/1/012020
2009IN02 Phys.Rev. C 80, 034321 (2009) I.Inci, C.E.Alonso, J.M.Arias, L.Fortunato, A.Vitturi Coherent state approach to the interacting boson model: Test of its validity in the transitional region
doi: 10.1103/PhysRevC.80.034321
2009TU04 Phys.Atomic Nuclei 72, 960 (2009) Quadrupole moments of some nuclei around the mass of A ∼ 80: 76, 78, 80, 82, 84Kr and neighboring Se isotopes NUCLEAR STRUCTURE 76,78,80,82,84Kr, 74,76,78,80,82Se;calculated quadrupole moments, B(E2). Interaction Boson Model (IBM).
doi: 10.1134/S1063778809060088
2008BO15 Phys.Rev. C 77, 044302 (2008) I.Boztosun, D.Bonatsos, I.Inci Analytical solutions of the Bohr Hamiltonian with the Morse potential 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, 140,148,150Nd, 140,142,152,154Sm, 142,144,152,154,156,158,160,162Gd, 154,158,160,162,164,166Dy, 156,160,162,164,166,168,170Er, 164,166,168,170,172,174,176,178Yb, 168,170,172,174,176,178,180Hf, 176,178,180,182,184,186W, 186,188,190,192,194,196,198,200Pt; 178,180,184,186,188Os, 228Ra, 228,230,232Th, 232,234,236,238U, 238,240,242Pu, 248Cm, 250Cf, calculated Bohr Hamilton and Morse Potential, angular momenta, bandheads and energy spacings of g.s., first 2+ and 4+ states.
doi: 10.1103/PhysRevC.77.044302
2008TU06 Phys.Atomic Nuclei 71, 1918 (2008) Comparing some predictions between Davidson-like potentials and interacting boson model: X(5) behavior of even-even 128-140Nd isotopes
doi: 10.1134/S1063778808110082
2007IN01 Turk.J.Phys. 30, 493 (2007) IBM-2 Calculations of Selected Even-Even Ruthenium Nuclei NUCLEAR STRUCTURE 102,104,106,108,110Ru; calculated levels, J, π, δ. Interacting boson model.
2007IN02 Turk.J.Phys. 30, 503 (2007) IBM-2 Calculations of Selected Even-Even Palladium Nuclei NUCLEAR STRUCTURE 102,104,106,108,110Pd; calculated levels, J, π, δ. Interacting boson model.
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