NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = P.E.Georgoudis Found 4 matches. 2021GE06 Nucl.Phys. A1015, 122297 (2021) Conformal symmetry in nuclear structure
doi: 10.1016/j.nuclphysa.2021.122297
2013BO24 Phys.Rev. C 88, 034316 (2013) D.Bonatsos, P.E.Georgoudis, N.Minkov, D.Petrellis, C.Quesne Bohr Hamiltonian with a deformation-dependent mass term for the Kratzer 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, 154,156,158,160,162,164,166Dy, 156,160,162,164,166,168,170Er, 162,164,166,168,170,172,174,176,178Yb, 166,168,170,172,174,176,178,180Hf, 176,178,180,182,184,186W, 176,178,180,184,186,188,190Os, 186,188,190,192,194,196,198,200Pt, 228Ra, 228,230,232Th, 232,234,236,238U, 238,240,242Pu, 248Cm, 250Cf; calculated levels, J, π, ground, β and γ bands, B(E2), ratios of level energies of yrast bands and low-lying positive-parity levels. Deformation-dependent mass (DDM) Bohr Hamiltonian with Kratzer potential obtained for γ-unstable, axially symmetric prolate deformed, and triaxial nuclei. Techniques of supersymmetric quantum mechanics (SUSYQM).
doi: 10.1103/PhysRevC.88.034316
2012BO22 J.Phys.:Conf.Ser. 366, 012017 (2012) D.Bonatsos, P.E.Georgoudis, D.Lenis, N.Minkov, C.Quesne Fixing the moment of inertia in the Bohr Hamiltonian through Supersymmetric Quantum Mechanics NUCLEAR STRUCTURE 162Dy, 238U; calculated energy levels, J of gs band, deformation of states using Bohr-Mottelson model. Compared with data.
doi: 10.1088/1742-6596/366/1/012017
2011BO12 Phys.Rev. C 83, 044321 (2011) D.Bonatsos, P.E.Georgoudis, D.Lenis, N.Minkov, C.Quesne Bohr Hamiltonian with a deformation-dependent mass term for the Davidson 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, 154,156,158,160,162,164,166Dy, 156,160,162,164,166,168,170Er, 162,164,166,168,170,172,174,176,178Yb, 166,168,170,172,174,176,178,180Hf, 176,178,180,182,184,186W, 176,178,180,184,186,188,190Os, 186,188,190,192,194,196,198,200Pt, 228Ra, 228,230,232Th, 232,234,236,238U, 238,240,242Pu, 248Cm, 250Cf; calculated levels, J, π, B(E2). Bohr collective Hamiltonian, β2 deformation dependent mass, curved space, Davidson potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.044321
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