NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.Bonatsos Found 90 matches. 2023BO09 J.Phys.(London) G50, 075105 (2023) D.Bonatsos, A.Martinou, S.K.Peroulis, T.J.Mertzimekis, N.Minkov Signatures for shape coexistence and shape/phase transitions in even-even nuclei NUCLEAR STRUCTURE 40Ar, 40,42Ca, 70,72Ge, 72Se, 96,98Sr, 98,100Zr, 100,102Mo, 104Ru, 110Pd, 112,116Cd, 114,116,118Sn, 126Xe, 148,150Nd, 152,154Sm, 152,154,156,158Gd, 166Er, 172,174Yb, 186,192Os, 196Pt; analyzed available data; deduced systematics of B(E2) transition rates connecting the first excited 0+2 state of the ground state band in even–even nuclei, shape coexistence of the ground state band.
doi: 10.1088/1361-6471/acd70b
2023HA02 Nucl.Phys. A1030, 122576 (2023) M.M.Hammad, M.M.Yahia, D.Bonatsos Triaxial nuclei and analytical solutions of the conformable fractional Bohr Hamiltonian with some exponential-type potentials NUCLEAR STRUCTURE 114,116Pd, 126,128Xe, 192,194Pt; calculated normalized B(E2) transitions and spectra. Comparison with the experimental data and theoretical predictions of Kratzer potential.
doi: 10.1016/j.nuclphysa.2022.122576
2022AL19 Phys.Rev. C 106, 054304 (2022) P.Alexa, M.Abolghasem, G.Thiamova, D.Bonatsos, T.R.Rodriguez, P.-G.Reinhard Macroscopic and microscopic description of phase transition in cerium isotopes NUCLEAR STRUCTURE 146,148Ce, 150Ce; calculated levels, J, π, B(E2), ground state deformation. 142,144,146,148,150,152Ce; calculated potential energy surface, potential energy curves. Calculations in the framework of the macroscopic algebraic collective model (ACM) and two microscopic approaches - Skyrme-Hartree-Fock+Bardeen-Cooper-Schrieffer (BCS) and the symmetry conserving configuration mixing method (SCCM) with Gogny energy density functionals. Systematics of the experimental energy ratios for 0+, 2+, 4+, 6+ levels of Ce, Nd, Sm, Gd and Dy isotopes. Comparison with experimental data.
doi: 10.1103/PhysRevC.106.054304
2022BO05 Phys.Lett. B 829, 137099 (2022) D.Bonatsos, K.E.Karakatsanis, A.Martinou, T.J.Mertzimekis, N.Minkov Microscopic origin of shape coexistence in the N=90, Z=64 region NUCLEAR STRUCTURE 176,178,180,182,184,186,188,190,192,194,196,198Po, 104,106,108,110,112,114,116,118,120,122,124,126,128,130Te, 70,72,74,76,78,80,82,84,86,88Zr; calculated single particle states using standard covariant density functional theory; deduced shape coexistence.
doi: 10.1016/j.physletb.2022.137099
2022BO16 Phys.Rev. C 106, 044323 (2022) D.Bonatsos, K.E.Karakatsanis, A.Martinou, T.J.Mertzimekis, N.Minkov Islands of shape coexistence from single-particle spectra in covariant density functional theory NUCLEAR STRUCTURE 68,70,90Zn, 70,72,92Ge, 72,74,92,94Se, 74,76,94,96Kr, 68,70,72,74,76,78,80,82,84,86,96,98Sr, 72,74,76,78,80,82,84,86,88,98,100Zr, 100,102Mo, 102,104Ru, 104,106Pd, 106,108Cd, 104,106,108,110,112,114,116,118,120,122,124,126,128,130,142,144,146,148Te, 144,146,148,150Xe, 146,148,150,152Ba, 148,150,152,154Ce, 150,152,154,156Nd, 152,154,156,158Sm, 154,156,158,160Gd, 156,158,160,162Dy, 158,160,162,164Er, 160,162,164,166Yb, 162,164,166,168Hf, 164,166,168,170W, 166,168,170,172Os, 170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200Pt, 172,174,176,178,180,182,184,186,188,190,192,194Hg, 174,176,178,180,182,184,186,188,190,192,194,196Pb, 176,178,180,182,184,186,188,190,192,194,196,198Po; calculated proton single-particle energy levels, potential energy surface. Covariant density functional theory with the DDME2 functional. Searched for regions with p-h excitations which are attributed to the shape coexistence. Islands of shape coexistence are identified at Z=82 and Z=50, and around the relevant neutron midshells N=104 and N=66.
doi: 10.1103/PhysRevC.106.044323
2022HA30 Nucl.Phys. A1028, 122540 (2022) M.M.Hammad, A.Martinou, D.Bonatsos Algebraic solutions for o(12) ← → u(2) (x) u(10) quantum phase transitions in the proton-neutron interacting boson model
doi: 10.1016/j.nuclphysa.2022.122540
2021BO08 Nucl.Phys. A1009, 122158 (2021) D.Bonatsos, I.E.Assimakis, A.Martinou, S.Sarantopoulou, S.K.Peroulis, N.Minkov Energy differences of ground state and γ1ands as a hallmark of collective behavior
doi: 10.1016/j.nuclphysa.2021.122158
2021MA25 Eur.Phys.J. A 57, 84 (2021) A.Martinou, D.Bonatsos, T.J.Mertzimekis, K.E.Karakatsanis, I.E.Assimakis, S.K.Peroulis, S.Sarantopoulou, N.Minkov The islands of shape coexistence within the Elliott and the proxy-SU(3) Models NUCLEAR STRUCTURE N=120-190; analyzed available data; deduced nucleon number systematics.
doi: 10.1140/epja/s10050-021-00396-w
2021MA26 Eur.Phys.J. A 57, 83 (2021) A.Martinou, D.Bonatsos, K.E.Karakatsanis, S.Sarantopoulou, I.E.Assimakis, S.K.Peroulis, N.Minkov Why nuclear forces favor the highest weight irreducible representations of the fermionic SU(3) symmetry NUCLEAR STRUCTURE 208Pb; analyzed available data; deduced prolate to oblate shape transitions.
doi: 10.1140/epja/s10050-021-00395-x
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
2020BO16 Eur.Phys.J. Special Topics 229, 2367 (2020) D.Bonatsos, A.Martinou, S.Sarantopoulou, I.E.Assimakis, S.Peroulis, N.Minkov Parameter-free predictions for the collective deformation variables b and γ within the pseudo-SU(3) scheme NUCLEAR STRUCTURE 142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180Ce, 146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184Sm, 148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186Dy, 154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194Yb, 158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194W, 162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202Pt; calculated distribution of valence protons and valence neutrons, weight of irreducible representations, collective deformation parameters.
doi: 10.1140/epjst/e2020-000034-3
2020CA27 Phys.Rev. C 102, 054310 (2020) R.F.Casten, R.B.Cakirli, D.Bonatsos, K.Blaum Simple new signature of structure in deformed nuclei: Distinguishing the nature of axial asymmetry NUCLEAR STRUCTURE 154,156,158,160,162Gd, 158,160,162,164,166Dy, 162,164,168,170,172Er, 164,166,168,170,172,174,176Yb, 168,170,172,174,176,178,180Hf, 170,172,174,176,178,180,182,184,186,188W, 182,184,186,188,190,192Os, 186,188,190,192,194,196Pt; analyzed ratios of two γ-band to ground-band experimental transition energies as a function of spin, and ratios of the inertial parameters between the γ bands and the ground bands; deduced a new and robust signature of structure of well-deformed and transitional even-even nuclei.
doi: 10.1103/PhysRevC.102.054310
2020MA49 Eur.Phys.J. A 56, 239 (2020) A.Martinou, D.Bonatsos, N.Minkov, I.E.Assimakis, S.K.Peroulis, S.Sarantopoulou, J.Cseh Proxy-SU(3) symmetry in the shell model basis
doi: 10.1140/epja/s10050-020-00239-0
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
2017BO11 Phys.Rev. C 95, 064325 (2017) D.Bonatsos, I.E.Assimakis, N.Minkov, A.Martinou, R.B.Cakirli, R.F.Casten, K.Blaum Proxy-SU(3) symmetry in heavy deformed nuclei
doi: 10.1103/PhysRevC.95.064325
2017BO12 Phys.Rev. C 95, 064326 (2017) D.Bonatsos, I.E.Assimakis, N.Minkov, A.Martinou, S.Sarantopoulou, R.B.Cakirli, R.F.Casten, K.Blaum Analytic predictions for nuclear shapes, prolate dominance, and the prolate-oblate shape transition in the proxy-SU(3) model NUCLEAR STRUCTURE 112,114,116,118,120,122,124,126,128,130,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176Ba, 114,116,118,120,122,124,126,128,130,132,134,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178Ce, 116,118,120,122,124,126,128,130,132,134,136,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180Nd, 118,120,122,124,126,128,130,132,134,136,138,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182Sm, 120,122,124,126,128,130,132,134,136,138,140,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184Gd, 122,124,126,128,130,132,134,136,138,140,142,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186Dy, 124,126,128,130,132,134,136,138,140,142,146,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Er, 126,128,130,132,134,136,138,140,142,146,148,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190Yb, 128,130,132,134,136,138,140,142,146,148,150,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192Hf, 130,132,134,136,138,140,142,146,148,150,152,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194W, 132,134,136,138,140,142,146,148,150,152,154,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196Os, 134,136,138,140,142,146,148,150,152,154,156,178,180,182,184,186,188,190,192,194,196,198Pt; calculated β and γ deformations using a new approximate analytic parameter-free proxy-SU(3) model. Comparison with empirical results.
doi: 10.1103/PhysRevC.95.064326
2017BO16 Eur.Phys.J. A 53, 148 (2017) Prolate over oblate dominance in deformed nuclei as a consequence of the SU(3) symmetry and the Pauli principle
doi: 10.1140/epja/i2017-12346-x
2017KO03 Phys.Rev. C 95, 014309 (2017) T.Konstantinopoulos, P.Petkov, A.Goasduff, T.Arici, A.Astier, L.Atanasova, M.Axiotis, D.Bonatsos, P.Detistov, A.Dewald, M.J.Eller, V.Foteinou, A.Gargano, G.Georgiev, K.Gladnishki, A.Gottardo, S.Harissopulos, H.Hess, S.Kaim, D.Kocheva, A.Kusoglu, A.Lagoyannis, J.Ljungvall, R.Lutter, I.Matea, B.Melon, T.J.Mertzimekis, A.Nannini, C.M.Petrache, A.Petrovici, G.Provatas, P.Reiter, M.Rocchini, S.Roccia, M.Seidlitz, B.Siebeck, D.Suzuki, N.Warr, H.De Witte, T.Zerrouki Lifetime measurements in 100Ru NUCLEAR REACTIONS 88Sr(14C, 2n), E=40, 46 MeV; measured Eγ, half-lives of 2+, 4+, 6+ and 8+ yrast levels by recoil-distance Doppler shift (RDDS) and Doppler-shift attenuation method (DSAM) using ORGAM array and eight detectors from Miniball array at 15 MV Tandem accelerator of the ALTO laboratory in Orsay. 100Ru; deduced levels, B(E2), not the best candidate for E(5) symmetry. Comparison with excited Vampir, shell-model calculations, and theoretical E(5) level scheme.
doi: 10.1103/PhysRevC.95.014309
2015BO05 Phys.Rev. C 91, 054315 (2015) D.Bonatsos, A.Martinou, N.Minkov, S.Karampagia, D.Petrellis Octupole deformation in light actinides within an analytic quadrupole octupole axially symmetric model with a Davidson potential NUCLEAR STRUCTURE 222,224,226Ra, 224,226Th; calculated levels, J, π, B(E1), BE(2), B(E3). Analytic quadrupole octupole axially (AQOA) symmetric model using Davidson potential. Bohr collective Hamiltonian, and quadrupole plus octupole deformation. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.054315
2015BO10 J.Phys.(London) G42, 095104 (2015) D.Bonatsos, N.Minkov, D.Petrellis Bohr Hamiltonian with a deformation-dependent mass term: physical meaning of the free parameter
doi: 10.1088/0954-3899/42/9/095104
2015CA17 J.Phys.(London) G42, 095102 (2015) M.Capak, D.Petrellis, B.Gonul, D.Bonatsos Analytical solutions for the Bohr Hamiltonian with the Woods-Saxon potential NUCLEAR STRUCTURE 150Nd, 152,154Sm, 154,156,158Gd, 156,158,160Dy, 160,162,164Er, 162,164,166,168,170,172,174,176Yb, 166,168,170,172,174,176,178Hf, 176,178,180W, 176,178,180,182,184Os, 228Ra, 228,230,232Th, 232,234,236,238U, 240,242Pu, 248Cm, 160,162Gd, 162,164,166Dy, 166,168Er, 178Yb, 180Hf, 182,184,186W, 186,188Os, 238Pu, 118,120,122,124,126,128,130,132,134Xe; calculated nuclear potential parameters. Comparison with available data.
doi: 10.1088/0954-3899/42/9/095102
2015KA18 Phys.Rev. C 91, 054325 (2015) S.Karampagia, D.Bonatsos, R.F.Casten Regularity and chaos in 0+ states of the interacting boson model using quantum measures
doi: 10.1103/PhysRevC.91.054325
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
2013BO27 Phys.Rev. C 88, 054309 (2013) D.Bonatsos, S.Karampagia, R.B.Cakirli, R.F.Casten, K.Blaum, L.Amon Susam Emergent collectivity in nuclei and enhanced proton-neutron interactions NUCLEAR STRUCTURE Z=50-82, N=82-126; analyzed empirical values of proton-neutron interaction Vpn for even and odd Z nuclei, E(4+)/E(2+) values for even A nuclei; calculated average spatial overlaps (for deformation ϵ=0.22) for proton and neutron orbitals, Nilsson diagrams; deduced enhancement of the large empirical values of p-n interactions along the Z=N line indicative of collectivity, shape changes, and the saturation of deformation. Pseudoshell approach to heavy nuclei.
doi: 10.1103/PhysRevC.88.054309
2012BO02 Rom.J.Phys. 57, 49 (2012) Conformal Maps and Group Contractions in Nuclear Structure Models
2012BO21 J.Phys.:Conf.Ser. 366, 012005 (2012) Group contractions and conformal maps in nuclear structure
doi: 10.1088/1742-6596/366/1/012005
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
2012BO23 J.Phys.:Conf.Ser. 366, 012025 (2012) D.Bonatsos, S.Karampagia, R.F.Casten Analytic derivation of the Alhassid-Whelan arc of regularity
doi: 10.1088/1742-6596/366/1/012025
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
2011BO15 Phys.Rev. C 83, 054313 (2011) D.Bonatsos, S.Karampagia, R.F.Casten Analytic derivation of an approximate SU(3) symmetry inside the symmetry triangle of the interacting boson approximation model
doi: 10.1103/PhysRevC.83.054313
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
2011YI01 Phys.Rev. C 83, 014303 (2011) Bohr Hamiltonian with Davidson potential for triaxial nuclei NUCLEAR STRUCTURE 128,130,132Xe; calculated levels, J, π, B(E2). Bohr collective Hamiltonian, Davidson potential in β and a steep harmonic oscillator in γ. Shape transition from a triaxial vibrator to the rigid triaxial rotator. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.014303
2010BO01 Phys.Rev.Lett. 104, 022502 (2010) D.Bonatsos, E.A.McCutchan, R.F.Casten SU(3) Quasidynamical Symmetry Underlying the Alhassid-Whelan Arc of Regularity
doi: 10.1103/PhysRevLett.104.022502
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
2009BO23 Phys.Rev. C 80, 034311 (2009); Erratum Phys.Rev. C 80, 049902 (2009) D.Bonatsos, E.A.McCutchan, R.F.Casten, R.J.Casperson, V.Werner, E.Williams Regularities and symmetries of subsets of collective 0+ states
doi: 10.1103/PhysRevC.80.034311
2008BO13 Phys.Rev.Lett. 100, 142501 (2008) D.Bonatsos, E.A.McCutchan, R.F.Casten, R.J.Casperson Simple Empirical Order Parameter for a First-Order Quantum Phase Transition in Atomic Nuclei
doi: 10.1103/PhysRevLett.100.142501
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
2008BO22 Phys.Rev.Lett. 101, 022501 (2008) D.Bonatsos, E.A.McCutchan, R.F.Casten Unified Description of 0+ States in a Large Class of Nuclear Collective Models NUCLEAR STRUCTURE 150Nd, 152Sm, 154,156,158Gd; calculated level energies for 0+ states using collective models. Compared results to data.
doi: 10.1103/PhysRevLett.101.022501
2007BO45 Rom.J.Phys. 52, 779 (2007) D.Bonatsos, D.Lenis, D.Petrellis, P.A.Terziev, I.Yigitoglu γ-Rigid Solution of the Bohr Hamiltonian for γ=30 degrees Compared to the E(5) Critical Point Symmetry NUCLEAR STRUCTURE 128,130,132Xe; calculated level energies and B(E2) using the Z(4) model.
2007BO46 Phys.Rev. C 76, 064312 (2007) D.Bonatsos, E.A.McCutchan, N.Minkov, R.F.Casten, P.Yotov, D.Lenis, D.Petrellis, I.Yigitoglu Exactly separable version of the Bohr Hamiltonian with the Davidson potential NUCLEAR STRUCTURE 154Sm, 156,158,160,162Gd, 158,160,162,164,166Dy, 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, 180,182,184,186,188Os, 228Ra, 228,230,232Th, 232,234,236,238U, 238,240,242Pu, 248Cm, 250Cf; calculated excitation energy ratios, angular momenta, B(E2) ratios, bandhead energies, deformation parameters using Bohr Hamiltonian with Davidson Potential, compared with experimental values.
doi: 10.1103/PhysRevC.76.064312
2007MC03 Phys.Rev. C 76, 024306 (2007) E.A.McCutchan, D.Bonatsos, N.V.Zamfir, R.F.Casten Staggering in γ-band energies and the transition between different structural symmetries in nuclei
doi: 10.1103/PhysRevC.76.024306
2007MC04 Phys.Atomic Nuclei 70, 1462 (2007) E.A.McCutchan, D.Bonatsos, N.V.Zamfir Connecting the X(5)-β2, X(5)-β4, and X(3) models to the shape/phase transition region of the interacting boson model NUCLEAR STRUCTURE 146Ce, 158Er, 172,174,176Os, 186Pt; calculated level energies, B(E2) using geometric models and IBA. Compared the results from the models to each other and to experimental data.
doi: 10.1134/S1063778807080236
2007MI30 Phys.Atomic Nuclei 70, 1470 (2007) N.Minkov, S.B.Drenska, P.Yotov, D.Bonatsos, W.Scheid Collective states of odd nuclei in a model with quadrupole-octupole degrees of freedom NUCLEAR STRUCTURE 219,221,223,225Fr, 223,225Th; calculated level energies of positive and negative parity bands using the collective axial quadrupole-octupole Hamiltonian.
doi: 10.1134/S1063778807080248
2007MI33 Phys.Rev. C 76, 034324 (2007) N.Minkov, S.Drenska, P.Yotov, S.Lalkovski, D.Bonatsos, W.Scheid Coherent quadrupole-octupole modes and split parity-doublet spectra in odd-A nuclei NUCLEAR STRUCTURE Nd, Pm, Sm, eu, Gd, Tb, Dy, Ho, Fr, Ra, Ac, Th, Pa, U, Np, Pu, Am, Cm, Bk; calculated level energies, parity doublet splittings, B(E1), B(E2) using a collective model. Compared results to available data.calculated energies.
doi: 10.1103/PhysRevC.76.034324
2006BO02 Phys.Lett. B 632, 238 (2006) D.Bonatsos, D.Lenis, D.Petrellis, P.A.Terziev, I.Yigitoglu X(3): an exactly separable γ-rigid version of the X(5) critical point symmetry NUCLEAR STRUCTURE 186Pt, 172Os, 156Dy, 154Gd, 152Sm, 150Nd; calculated ground and vibrational bands level energies, B(E2), critical point symmetry, shape transition features. Analytic quadrupole octupole axially symmetric model, comparison with data.
doi: 10.1016/j.physletb.2005.10.060
2006BO24 Phys.Rev. C 74, 044306 (2006) D.Bonatsos, D.Lenis, N.Pietralla, P.A.Terziev γ-soft analog of the confined β-soft rotor model NUCLEAR STRUCTURE 128,130Xe; calculated levels, J, π, B(E2), symmetry features. γ-soft analog of the confined β-soft rotor model.
doi: 10.1103/PhysRevC.74.044306
2006FO05 Phys.Rev. C 73, 044310 (2006) R.Fossion, D.Bonatsos, G.A.Lalazissis E(5), X(5), and prolate to oblate shape phase transitions in relativistic Hartree-Bogoliubov theory NUCLEAR STRUCTURE 96,98,100,102,104,106,108,110,112,114Pd, 118,120,122,124,126,128,130,132,134Xe, 118,120,122,124,126,128,130,132,134,136,138Ba, 144,146,148,150,152,154,156Nd, 146,148,150,152,154,156,158Sm, 148,150,152,154,156Gd, 150,152,154,156,158Dy, 180Hf, 182,184,186W, 188,190,192,194,196,198,200Os, 184,186W, 188,190,192,194,196,198,200,202Pt, 198,200Hg; calculated potential energy surfaces; deduced symmetry and shape transition features. Relativistic mean-field approach, NL3 force.
doi: 10.1103/PhysRevC.73.044310
2006LE09 Phys.Lett. B 633, 474 (2006) Parameter-free solution of the Bohr Hamiltonian for actinides critical in the octupole mode NUCLEAR STRUCTURE 218,220,222,224,226,228Ra, 220,222,224,226,228,230,232,234Th; calculated ground and vibrational bands level energies, B(E1), B(E2), B(E3), critical point symmetry, shape transition features. Analytic quadrupole octupole axially symmetric model, comparison with data.
doi: 10.1016/j.physletb.2005.12.016
2006MC04 Phys.Rev. C 74, 034306 (2006) E.A.McCutchan, D.Bonatsos, N.V.Zamfir Connecting the X(5)-β2, X(5)-β4, and X(3) models to the shape/phase-transition region of the interacting boson model NUCLEAR STRUCTURE 146Ce, 158Er, 172,174,176Os, 186Pt; calculated levels, J, π, symmetry features.
doi: 10.1103/PhysRevC.74.034306
2006MI11 Phys.Rev. C 73, 044315 (2006) N.Minkov, P.Yotov, S.Drenska, W.Scheid, D.Bonatsos, D.Lenis, D.Petrellis Nuclear collective motion with a coherent coupling interaction between quadrupole and octupole modes NUCLEAR STRUCTURE 150Nd, 152Sm, 154Gd, 156Dy; calculated energy vs spin, transition probabilities for alternating-parity rotational bands, coupling of quadrupole and octupole degrees of freedom.
doi: 10.1103/PhysRevC.73.044315
2005BO18 Phys.Rev. C 71, 064309 (2005) D.Bonatsos, D.Lenis, N.Minkov, D.Petrellis, P.Yotov Analytic description of critical-point actinides in a transition from octupole deformation to octupole vibrations NUCLEAR STRUCTURE 220,222,224,226,228,230,232,234Th, 218,220,222,224,226,228,230Ra; calculated ground and vibrational bands level energies, B(E1), B(E2), critical point symmetry, shape transition features.Analytic quadrupole octupole axially symmetric model, comparison with data.
doi: 10.1103/PhysRevC.71.064309
2005BO30 Phys.Lett. B 621, 102 (2005) D.Bonatsos, D.Lenis, D.Petrellis, P.A.Terziev, I.Yigitoglu γ-rigid solution of the Bohr Hamiltonian for γ = 30 degrees compared to the E(5) critical point symmetry NUCLEAR STRUCTURE 128,130,132Xe; analyzed levels, J, π, B(E2); deduced symmetry features.
doi: 10.1016/j.physletb.2005.06.047
2004BO02 Phys.Rev. C 69, 014302 (2004) D.Bonatsos, D.Lenis, N.Minkov, P.P.Raychev, P.A.Terziev Sequence of potentials lying between the U(5) and X(5) symmetries NUCLEAR STRUCTURE 148Nd, 160Yb, 158Er; calculated ground and vibrational bands level energies, J, π, B(E2). Harmonic oscillator, X(5) symmetries.
doi: 10.1103/PhysRevC.69.014302
2004BO14 Phys.Rev. C 69, 044316 (2004) D.Bonatsos, D.Lenis, N.Minkov, P.P.Raychev, P.A.Terziev Sequence of potentials interpolating between the U(5) and E(5) symmetries NUCLEAR STRUCTURE 100Pd, 98Ru; calculated levels, J, π, B(E2). Bohr collective Hamiltonian, extensions of E(5) model.
doi: 10.1103/PhysRevC.69.044316
2004BO15 Phys.Lett. B 588, 172 (2004) D.Bonatsos, D.Lenis, D.Petrellis, P.A.Terziev Z(5): critical point symmetry for the prolate to oblate nuclear shape phase transition NUCLEAR STRUCTURE 192,194,196Pt; analyzed transitions B(E2); critical point symmetry, shape transition features.
doi: 10.1016/j.physletb.2004.03.029
2004BO19 Phys.Lett. B 584, 40 (2004) D.Bonatsos, D.Lenis, N.Minkov, D.Petrellis, P.P.Raychev, P.A.Terziev Ground state bands of the E(5) and X(5) critical symmetries obtained from Davidson potentials through a variational procedure
doi: 10.1016/j.physletb.2004.01.018
2004BO33 Phys.Rev. C 70, 024305 (2004) D.Bonatsos, D.Lenis, N.Minkov, D.Petrellis, P.P.Raychev, P.A.Terziev E(5) and X(5) critical point symmetries obtained from Davidson potentials through a variational procedure
doi: 10.1103/PhysRevC.70.024305
2004BO38 Yad.Fiz. 67, 1795 (2004); Phys.Atomic Nuclei 67, 1767 (2004) D.Bonatsos, D.Lenis, N.Minkov, P.P.Raychev, P.A.Terziev Extended E(5) and X(5) Symmetries: Series of Models Providing Parameter-Independent Predictions
doi: 10.1134/1.1811176
2002BO48 Phys.Rev. C 66, 054306 (2002) D.Bonatsos, B.A.Kotsos, P.P.Raychev, P.A.Terziev Rotationally invariant Hamiltonians for nuclear spectra based on quantum algebras NUCLEAR STRUCTURE 222,224,226,228,230,232,234Th; calculated level energies. Quantum algebra, rotationally invariant Hamiltonian. Comparison with data.
doi: 10.1103/PhysRevC.66.054306
2001MI10 Phys.Rev. C63, 044305 (2001) N.Minkov, S.B.Drenska, P.P.Raychev, R.P.Roussev, D.Bonatsos ' Beat ' Patterns for the Odd-Even Staggering in Octupole Bands from a Quadrupole-Octupole Hamiltonian
doi: 10.1103/PhysRevC.63.044305
2001MI26 Yad.Fiz. 64, No 6, 1173 (2001); Phys.Atomic Nuclei 64, 1098 (2001) N.Minkov, S.B.Drenska, P.P.Raychev, R.P.Roussev, D.Bonatsos Rotations of Nuclei with Reflection Asymmetry Correlations
doi: 10.1134/1.1383624
2000BO34 Phys.Rev. C62, 024301 (2000); Erratum Phys.Rev. C63, 049902 (2001) D.Bonatsos, C.Daskaloyannis, S.B.Drenska, N.Karoussos, N.Minkov, P.P.Raychev, R.P.Roussev ΔI = 1 Staggering in Octupole Bands of Light Actinides: ' Beat ' Patterns NUCLEAR STRUCTURE 218,220,222Rn, 218,220,222,224,226Ra, 220,222,224,226,228Th; analyzed octupole bands transition energies; deduced beat patterns, possible mechanisms. Predictions of algebraic models discussed.
doi: 10.1103/PhysRevC.62.024301
2000BO44 Trans.Bulg.Nucl.Soc. 5, 18 (2000) D.Bonatsos, N.Karoussos, C.Daskaloyannis, S.B.Drenska, N.Minkov, P.P.Raychev, R.P.Roussev, J.Maruani Symmetries in Nuclei, Molecules and Atomic Clusters
2000MI18 Phys.Rev. C61, 064301 (2000) N.Minkov, S.B.Drenska, P.P.Raychev, R.P.Roussev, D.Bonatsos Ground-γ Band Mixing and Odd-Even Staggering in Heavy Deformed Nuclei NUCLEAR STRUCTURE 156Gd, 156,160,162Dy, 162,164,166Er, 170Yb, 228,232Th; analyzed vibrational bands odd-even staggering effect, role of band mixing. Vector boson model with SU(3) dynamical symmetry.
doi: 10.1103/PhysRevC.61.064301
2000MI29 Trans.Bulg.Nucl.Soc. 5, 192 (2000) N.Minkov, S.Drenska, P.Raychev, R.Roussev, D.Bonatsos Ground-γ Band Mixing and ΔL = 1 Staggering in Heavy Deformed Nuclei NUCLEAR STRUCTURE 164,166Er; analyzed rotational band level staggering; deduced ground-γ band mixing. Vector boson model.
1999BO43 Prog.Part.Nucl.Phys. 43, 537 (1999) Quantum Groups and Their Applications in Nuclear Physics
doi: 10.1016/S0146-6410(99)00100-3
1999MI23 Phys.Rev. C60, 034305 (1999) N.Minkov, S.B.Drenska, P.P.Raychev, R.P.Roussev, D.Bonatsos Ground-γ Band Coupling in Heavy Deformed Nuclei and SU(3) Contraction Limit NUCLEAR STRUCTURE 152,154Sm, 154,156,158,160Gd, 158,160,162,164Dy, 162,164,166,168,170Er, 168,170,172,174,176Yb, 174,178Hf, 182,184,186W, 230,232Th, 234,238U; analyzed ground, vibrational bands levels, interband, intraband transitions B(E2); deduced band mixing features. Vector-boson model with SU(3) dynamical symmetry.
doi: 10.1103/PhysRevC.60.034305
1997MI10 Phys.Rev. C55, 2345 (1997) N.Minkov, S.B.Drenska, P.P.Raychev, R.P.Roussev, D.Bonatsos Broken SU(3) Symmetry in Deformed Even-Even Nuclei NUCLEAR STRUCTURE 164Dy, 164,166,168Er, 168,172Yb, 176,178Hf, 238U; calculated levels, transition ratios, energy rms factor. Collective vector-boson model.
doi: 10.1103/PhysRevC.55.2345
1996BO31 Roum.J.Phys. 41, 109 (1996) D.Bonatsos, C.Daskaloyannis, P.Kolokotronis, D.Lenis Quantum Algebras in Nuclear Structure
1996MI19 J.Phys.(London) G22, 1633 (1996) N.Minkov, S.B.Drenska, P.P.Raychev, R.P.Roussev, D.Bonatsos The SU(q)(2) Rotator Model in Excited Collective Bands of Even Deformed Nuclei NUCLEAR STRUCTURE 152,154Sm, 154,156,158,160Gd, 160,162,164Dy, 160,162,164,166,168,170Er, 166,168,170,172Yb, 172,174,176,178,180Hf, 178,180,182,184W, 232Th, 232,234U; analyzed (β)-, (γ)-bands levels, B(λ) data. Rotator SU(q)(2) model.
doi: 10.1088/0954-3899/22/11/010
1994BO21 Phys.Rev. C50, 497 (1994) D.Bonatsos, C.Daskaloyannis, A.Faessler, P.P.Raychev, R.P.Roussev Quantum Algebraic Description of Vibrational and Transitional Nuclear Spectra NUCLEAR STRUCTURE 150,152,154Sm, 152,154,158Gd, 154,156,162Dy, 156,158,166Er; calculated levels. Quantum algebraic description, SU(q)(2) model.
doi: 10.1103/PhysRevC.50.497
1994PR07 J.Phys.(London) G20, 1209 (1994); Erratum J.Phys.(London) G21, 591 (1995) C.Providencia, L.Brito, J.da Providencia, D.Bonatsos, D.P.Menezes The q-Deformed Moszkowski Model: High-spin states
doi: 10.1088/0954-3899/20/8/011
1992BO04 Nucl.Phys. A539, 189 (1992) M.Borromeo, D.Bonatsos, H.Muther, A.Polls Effects of Short-Range Correlations on the Self-Energy in the Optical Model of Finite Nuclei NUCLEAR STRUCTURE 16O; calculated interacting nucleon self-energy real, imaginary parts. Realistic one-boson-exchange potential, G-matrix approach.
doi: 10.1016/0375-9474(92)90266-M
1991BO05 Phys.Rev. C43, R952 (1991) D.Bonatsos, L.D.Skouras, J.Rikovska Successive Energy Ratios in Medium- and Heavy-Mass Nuclei as Indicators of Different Kinds of Collectivity NUCLEAR STRUCTURE A=74-248; analyzed level energy ratio systematics; deduced different kinds of collectivity.
doi: 10.1103/PhysRevC.43.R952
1991BO06 J.Phys.(London) G17, 63 (1991) D.Bonatsos, L.D.Skouras, J.Rikovska Tests of Phenomenological Collective Models Based on Energy Ratios and Staggering Systematics NUCLEAR STRUCTURE A=74-248; analyzed band structure, level systematics; deduced collective models applicability.
doi: 10.1088/0954-3899/17/1/006
1991BO11 J.Phys.(London) G17, L67 (1991) D.Bonatsos, S.B.Drenska, P.P.Raychev, R.P.Roussev, Yu.F.Smirnov Description of Superdeformed Bands by the Quantum Algebra SU(q)(2) NUCLEAR STRUCTURE 134,136Nd, 150Gd, 162,152Dy, 192,194Hg, 174Yb, 248Cm; analyzed level data; deduced superdeformed band features. Quantum SU(q)(2) algebra.
doi: 10.1088/0954-3899/17/5/003
1991BO13 J.Phys.(London) G17, 865 (1991) D.Bonatsos, L.D.Skouras, J.Rikovska Systematics of Energy Differences as Signs of Intruder Bands and Parameter Independent Tests of Interacting Boson Models for Octupole States NUCLEAR STRUCTURE 160,162,164Dy, 164,166,168Er, 166,168Yb, 232Th, 234U; calculated energy level difference ratio; analyzed systematics; deduced intruder bands role.
doi: 10.1088/0954-3899/17/6/009
1991BO45 J.Phys.(London) G17, 1803 (1991) D.Bonatsos, L.D.Skouras, P.Van Isacker, M.A.Nagarajan An Application of the Democratic Mapping to the sd and fp Shells NUCLEAR STRUCTURE 20Ne, 42Sc, 44Ti; calculated levels. Democratic mapping method.
doi: 10.1088/0954-3899/17/12/004
1990BO12 Nucl.Phys. A510, 55 (1990) Microscopic Calculation of the Optical-Model Potential for 40Ca NUCLEAR REACTIONS 40Ca(p, p), (n, n), E not given; calculated optical potential. Microscopic method, momentum space, realistic one-boson exchange potential.
doi: 10.1016/0375-9474(90)90287-V
1990BO47 Phys.Lett. 251B, 477 (1990) D.Bonatsos, E.N.Argyres, S.B.Drenska, P.P.Raichev, R.P.Roussev, Yu.F.Smirnov SU(q)(2) Description of Rotational Spectra and Its Relation to the Variable Moment of the Inertia Model NUCLEAR STRUCTURE 176Yb, 178Hf, 232U, 238Pu; calculated levels. SU(q)(2) description.
doi: 10.1016/0370-2693(90)90782-2
1989BO17 Nucl.Phys. A496, 23 (1989) Microscopic Calculation of the Optical-Model Potential for 16O NUCLEAR STRUCTURE 16O; calculated optical potential. Microscopic approach.
doi: 10.1016/0375-9474(89)90214-5
1988BO02 Phys.Lett. 200B, 1 (1988) Systematics of Odd-Even Staggering in γ-Bands as a Test for Phenomenological Collective Models NUCLEAR STRUCTURE 152,154,158,160Gd, 154,156,158,160,162Dy, 146,148,150,152,154Sm, 156,158,160,162,164,166,168Er, 160,162,164,166,168,170,172,174Yb, 190,188,186,184,182Os; analyzed levels, band structure; deduced γ-band staggering systematics. 232Th, 166Yb, 164Er, 178Hf; calculated odd spin to even spin level displacements. Phenomenological collective models.
doi: 10.1016/0370-2693(88)91098-2
1988BO11 J.Phys.(London) G14, 351 (1988) Unified Description of Deformed Even Nuclei in the SU(3) Limit of the Hybrid Model NUCLEAR STRUCTURE 230,232Th, 232,234,236,238U, 242,244Pu, 248Cm, 184,180W, 160,162,164Dy, 168,170,172Yb, 164,166,168,170Er, 180,174,176,178Hf; calculated levels. Moshinsky hybrid model.
doi: 10.1088/0305-4616/14/3/011
1988BO17 J.Phys.(London) G14, 569 (1988) Variable Moment of Inertia Models in the N(p)N(n) Scheme NUCLEAR STRUCTURE Z ≈ 50-100; analyzed ground state moment of inertia systematics; deduced model parameter dependence. Variable moment of inertia models.
doi: 10.1088/0305-4616/14/5/015
1988RI07 Phys.Lett. 211B, 259 (1988) Structure of Even-Even Actinides in the Interacting Boson Model and the N = 152 Subshell Closure NUCLEAR STRUCTURE 224,226,228,230Ra, 226,228,230,232,234Th, 232,234,236,238U, 238,240,242,246Pu, 244,246,248Cm, 250Cf; calculated levels, B(E2). Interacting boson model.
doi: 10.1016/0370-2693(88)90899-4
1987BO05 Phys.Lett. 187B, 1 (1987) Parameter Systematics of Variable Moment of Inertia Models in the N(p)N(n) Scheme NUCLEAR STRUCTURE 166,168,170,172,174,176,178,180,182Hf, 172,174,176,178,180,182,184,186W, 172,174,176,178,180,182,184,186,188,190,192Os, 182,184,186,188,190,192,194,196,198Pt; analyzed variable moment of inertia parameters vs valence proton-neutron product; deduced parameter systematics. VMI models.
doi: 10.1016/0370-2693(87)90061-X
1985BO20 Phys.Rev. C31, 2256 (1985) Simple Model for Backbending NUCLEAR STRUCTURE 154Gd, 162,156,164Er, 156Dy, 104Pd, 126Ba, 244Pu, 186Os; analyzed yrast level systematics; deduced aligned angular momentum increase, VMI, rotational superband parameters, interband interaction strengths.
doi: 10.1103/PhysRevC.31.2256
1984BO01 At.Data Nucl.Data Tables 30, 27 (1984) Energies of Ground-State Bands of Even Nuclei from Generalized Variable Moment of Inertia Models NUCLEAR STRUCTURE A=78-256; analyzed ground state band levels; deduced best fit parameters. Generalized variable moment of inertia models.
doi: 10.1016/0092-640X(84)90007-X
1984BO16 Phys.Rev. C29, 1879 (1984) Generalized Phenomenological Models of the Yrast Band NUCLEAR STRUCTURE 122,124,126,130,132,144,146Ba, 156,158,160,162,164,166,168,170Er, 152,154,156,158,160Gd, 158,160,162,164,166,168,170,172,174Yb, 172,174,176,178,180,182,184,186,188,190,192Os, 172,174,176,178,180,182,184,186,188W, 118,120,122,124,126,128Xe; analyzed yrast band systematics; deduced model parameter dependences. Generalized phenomenological models.
doi: 10.1103/PhysRevC.29.1879
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