NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = F.Iachello Found 88 matches. 2022GA03 Phys.Rev. C 105, 014305 (2022) N.Gavrielov, A.Leviatan, F.Iachello Zr isotopes as a region of intertwined quantum phase transitions NUCLEAR STRUCTURE 92,94,96,98,100,102,104,106,108,110Zr; calculated positive-parity levels up to 12+, bands, B(E2), symmetries for the lowest 0+ and 2+ states, potential energy surface contour plots in the (β, γ) plane, S(2n), isotope shifts, ρ(E0), magnetic moments of the first 2+ states; deduced intertwined quantum phase transitions (IQPTs) for weakly deformed to prolate deformed and finally to γ-unstable nuclei, associated with the U(5), SU(3) and SO(6) dynamical symmetry limits of the IBM. Calculations based on definite symmetry-based framework, in the interacting boson model with configuration mixing (IBM-CM). Comparison with other theoretical calculations, and with experimental data.
doi: 10.1103/PhysRevC.105.014305
2022GA28 Phys.Rev. C 106, L051304 (2022) N.Gavrielov, A.Leviatan, F.Iachello Mixed configurations and intertwined quantum phase transitions in odd-mass nuclei NUCLEAR STRUCTURE 93,95,97,99,101,103,105Nb; calculated levels, J, π, B(E2), B(M1), percentage of the intruder component in the ground and first excited positive parity states, quadrupole moments, magnetic moments. 92Zr; calculated levels, J, π, B(E2), B(M1). Interacting boson-fermion model with configuration mixing. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.L051304
2021BI01 Nucl.Phys. A1006, 122077 (2021) Cluster structure of 20Ne: Evidence for D3h symmetry NUCLEAR STRUCTURE 20Ne; calculated B(E2), form factors, rms radii, energy levels, rotational bands, B(Eλ), cluster configurations with bi-pyramidal structure symmetry.
doi: 10.1016/j.nuclphysa.2020.122077
2021BI04 Nucl.Phys. A1010, 122193 (2021) Cluster structure of 21Ne and 21Na NUCLEAR STRUCTURE 21Ne, 21Na; calculated energy levels, J, π within the framework of the cluster shell model (CSM).
doi: 10.1016/j.nuclphysa.2021.122193
2021KO10 Phys.Rev. C 103, 044302 (2021) Nuclear matrix elements for Majoron-emitting double-β decay RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 110Pd, 116Cd, 124Sn, 128,130Te, 134,136Xe, 148,150Nd, 154Sm, 160Gd, 198Pt, 232Th, 238U(2β-); calculated nuclear matrix elements (NMEs) for Majoron-emitting neutrinoless double-beta decay, limits on the Majoron-neutrino coupling constants for neutrino-less ββ decay of 76Ge, 130Te and 136Xe. Calculations based on interacting Boson Model IBM-2.
doi: 10.1103/PhysRevC.103.044302
2020BI02 Prog.Part.Nucl.Phys. 110, 103735 (2020) Cluster structure of light nuclei NUCLEAR STRUCTURE 8,9Be, 9B, 16O; analyzed available data; deduced cluster structure of light nuclei within the framework of the algebraic cluster model (ACM) for nuclei.
doi: 10.1016/j.ppnp.2019.103735
2020GA01 Phys.Scr. 95, 24001 (2020) N.Gavrielov, A.Leviatan, F.Iachello Interplay between shape-phase transitions and shape coexistence in the Zr isotopes NUCLEAR STRUCTURE 90,92,94,96,98,100,102,104,106,108,110Zr; calculated energy levels, J, π, B(E2).
doi: 10.1088/1402-4896/ab456b
2019BI03 Phys.Rev.Lett. 122, 162501 (2019) Evidence for Triangular D'3h Symmetry in 13C NUCLEAR STRUCTURE 12,13C; calculated rotational spectra, energy levels, J, π, B(Eλ).
doi: 10.1103/PhysRevLett.122.162501
2019GA21 Phys.Rev. C 99, 064324 (2019) N.Gavrielov, A.Leviatan, F.Iachello Intertwined quantum phase transitions in the Zr isotopes NUCLEAR STRUCTURE 90,92,94,96,98,100,102,104,106,108,110Zr; calculated levels, J, π, B(E2), differences in rms charge radii, S(2n), and contour plots in (β, γ) plane of the lowest eigenpotential surface. Interacting boson model with configuration mixing. Comparison with experimental values. Discussed intertwined quantum phase transitions.
doi: 10.1103/PhysRevC.99.064324
2018DE12 Nucl.Phys. A973, 1 (2018) Cluster shell model: I. Structure of 9Be, 9B NUCLEAR STRUCTURE 9Be, 9B; calculated sp levels, J, π in cluster potentials with given symmetry (appropriate to 8Be, 12C, 16O), binding energy, Q, deformation, B(E1), B(E2), B(E3), B(E4), B(E5), B(M1), μ, quadrupole moment, rotational bands, form factors, inertia moment and its components, matter radius, radial matter distribution, β-decay log ft using CSM (Cluster Shell Model). Compared with data and with ab initio, phenomenological shell model, LCAO (Linear Combination of Atomic Orbitals).
doi: 10.1016/j.nuclphysa.2018.02.003
2017BI01 Nucl.Phys. A957, 154 (2017) The algebraic cluster model: Structure of 16O NUCLEAR STRUCTURE 16O; calculated levels, J, π, gs rotational band, vibrational bands, form factors, B(E1), B(E2), B(E3), B(E4), B(E6) for selected states using four-body clusters with both continuous and discrete symmetries. Form factors compared with available data.
doi: 10.1016/j.nuclphysa.2016.08.008
2017DE19 Nucl.Phys. A966, 158 (2017) V.Della Rocca, R.Bijker, F.Iachello Single-particle levels in cluster potentials NUCLEAR STRUCTURE 8Be, 12C, 16O; calculated structure, cluster density distribution using α-cluster shell model and specific cluster potential. 9Be, 9B, 13C, 13N, 17O, 17F (cluster α nuclei plus or minus 1 nucleon); calculated single-particle levels, J, π vs deformation.
doi: 10.1016/j.nuclphysa.2017.06.032
2017ZH13 Phys.Rev. C 95, 034306 (2017) Two-nucleon transfer reactions as a test of quantum phase transitions in nuclei NUCLEAR REACTIONS 152,154,156,158,160Gd, 148,150,152,154Sm, 146,148Nd(p, t), (t, p), E not given; 144,150Nd(t, p), E not given; calculated two-neutron transfer intensities using interacting boson model (IBM), and compared with experimental data; deduced quantum phase transition (QPT) between spherical U(5) and axially deformed SU(3) shapes.
doi: 10.1103/PhysRevC.95.034306
2017ZH25 Phys.Rev. C 95, 061304 (2017) Jacobi-type transitions in the interacting boson model NUCLEAR STRUCTURE 152,154,156,158,160,162Gd; calculated Jacobi-type transitions from axial to triaxial configurations, and excited state quantum phase transitions (ESQPT) using interacting boson model; deduced empirical evidence for such transitions in rotational spectra of 156,158,160,162Gd.
doi: 10.1103/PhysRevC.95.061304
2015BA12 Phys.Rev. C 91, 034304 (2015) 0νββ and 2νββ nuclear matrix elements in the interacting boson model with isospin restoration
doi: 10.1103/PhysRevC.91.034304
2015KO15 Phys.Rev. C 91, 064310 (2015) Phase-space factors and half-life predictions for Majoron-emitting β-β- decay RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 110Pd, 116Cd, 124Sn, 128,130Te, 134,136Xe, 148,150Nd, 154Sm, 160Gd, 198Pt, 232Th, 238U(2β-); calculated Phase space factors using screened exact finite size Coulomb wave functions, half-lives for Majoron-emitting double-beta decay, single electron spectra, summed electron spectra, and angular correlations between the two outgoing electrons for 136Xe 0νββM decay mode. Comparison with experimental data for half-lives.
doi: 10.1103/PhysRevC.91.064310
2015SP02 Phys.Rev.Lett. 114, 192504 (2015) M.Spieker, S.Pascu, A.Zilges, F.Iachello Origin of Low-Lying Enhanced E1 Strength in Rare-Earth Nuclei NUCLEAR STRUCTURE 142,144,146,148,150Nd, 148,150Sm, 156,160Gd, 162,164Dy; calculated B(E1) distributions. spdf interacting boson model calculations, comparison with experimental data.
doi: 10.1103/PhysRevLett.114.192504
2014BI04 Phys.Rev.Lett. 112, 152501 (2014) Evidence for Tetrahedral Symmetry in 16O NUCLEAR STRUCTURE 16O; analyzed energy levels, J, π, B(E3), B(E4), B(E6) values; deduced cluster states, rotational bands, tetrahedral symmetry.
doi: 10.1103/PhysRevLett.112.152501
2014KO18 Phys.Rev. C 89, 064319 (2014) Neutrinoless double-electron capture RADIOACTIVITY 124Xe, 152Gd, 156Dy, 164Er, 180W(2EC); calculated prefactors, nuclear matrix elements, half-lives for 0νϵϵ decay mode for light and heavy neutrino exchange. IBM-2 model and Argonne short-range correlation (SRC). NUCLEAR STRUCTURE 124Xe, 124Te, 152Gd, 152Sm, 156Dy, 156Gd, 164Er, 164Dy, 180W, 180Hf; calculated levels, J, π using microscopic interacting boson model (IBM-2). Comparison with experimental data.
doi: 10.1103/PhysRevC.89.064319
2013BA05 Phys.Rev. C 87, 014315 (2013) Nuclear matrix elements for double-β decay RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 110Pd, 116Cd, 124Sn, 128,130Te, 148,150Nd, 154Sm, 160Gd, 198Pt(2β-); calculated nuclear matrix elements, half-lives for neutrinoless and two-neutrino double-β decay; deduced limits on ν mass from experiments and calculations, gA, gV. Microscopic interacting boson model (IBM-2). Light neutrino and heavy neutrino exchange. Comparison with QRPA-Tu and ISM calculation.
doi: 10.1103/PhysRevC.87.014315
2013BA18 Phys.Rev. C 87, 057301 (2013) Neutrinoless double-positron decay and positron-emitting electron capture in the interacting boson model RADIOACTIVITY 58Ni, 64Zn, 78Kr, 96Ru, 106Cd, 124Xe, 130Ba, 136Ce(2β+), (2EC), (β+EC); calculated nuclear matrix elements for 0νββ, 0νϵβ, and 0νϵϵ decay modes, half-lives. Microscopic interacting boson model (IBM-2).
doi: 10.1103/PhysRevC.87.057301
2013KO08 Phys.Rev. C 87, 024313 (2013) Phase space factors for β+β+ decay and competing modes of double-β decay RADIOACTIVITY 78Kr, 96Ru, 106Cd, 124Xe, 130Ba, 136Ce(2β+), (β+EC), (2EC); 50Cr, 58Ni, 64Zn, 74Se, 84Sr, 92Mo, 102Pd, 112Sn, 120Te, 144Sm, 156Dy, 162Er, 168Yb, 174Hf, 184Os, 190Pt(β+EC), (2EC); 40Ca, 54Fe, 108Cd, 126Xe, 132Ba, 138Ce, 158Dy, 180W, 196Hg(2EC); calculated phase space factors, positron spectra, angular correlations between two outgoing positrons, effective nuclear matrix elements for 2νββ decay using Dirac wave functions with finite nuclear size and electron screening. Comparison with previous theoretical studies.
doi: 10.1103/PhysRevC.87.024313
2012BA30 Phys.Rev.Lett. 109, 042501 (2012) Limits on Neutrino Masses from Neutrinoless Double-β Decay RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 110Pd, 116Cd, 124Sn, 128,130Te, 136Xe, 148,150Nd, 154Sm, 160Gd, 198Pt(2β-); analyzed theoretical and experimental data; calculated neutrinoless nuclear matrix elements; deduced neutrino mass limits.
doi: 10.1103/PhysRevLett.109.042501
2012KO10 Phys.Rev. C 85, 034316 (2012) Phase-space factors for double-β decay RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 110Pd, 116Cd, 124Sn, 128Te, 130Te, 136Xe, 148Nd, 150Nd, 154Sm, 160Gd, 198Pt, 232Th, 238U(2β-); calculated phase-space factors, Single-electron spectra, summed energy spectra, half-lives, angular correlations, effective nuclear matrix elements for 2νββ and 0νββ decay modes. Exact Dirac wave functions with finite nuclear size and electron screening. Comparison with previous studies and experimental data.
doi: 10.1103/PhysRevC.85.034316
2009BA20 Phys.Rev. C 79, 044301 (2009) Neutrinoless double-β decay in the microscopic interacting boson model RADIOACTIVITY 76Ge, 82Se, 100Mo, 128,130Te, 136Xe, 150Nd, 154Sm(2β-); calculated neutrinoless double-beta decay nuclear matrix elements, dependence of matrix elements on neutron number, valence neutron pairs and proton number. Microscopic interacting boson model, shell model and quasiparticle random phase approximation (QRPA) calculations.
doi: 10.1103/PhysRevC.79.044301
2007CA01 Nucl.Phys. A781, 26 (2007) Analytic descriptions for transitional nuclei near the critical point
doi: 10.1016/j.nuclphysa.2006.10.032
2006FR09 Phys.Rev. C 73, 061302 (2006) A.Frank, P.Van Isacker, F.Iachello Phase transitions in configuration mixed models NUCLEAR STRUCTURE Cd, Pd, Ru, Mo, Zr, Sr; analyzed two-neutron separation energies, phase transition features.
doi: 10.1103/PhysRevC.73.061302
2005IA02 Int.J.Mod.Phys. E14, 137 (2005) Symmetry in nuclei NUCLEAR STRUCTURE 152Sm, 156Gd, 190Os, 191Ir, 196Au; analyzed levels, J, π, symmetry features.
doi: 10.1142/S0218301305002862
2005IA03 Nucl.Phys. A751, 329c (2005) Symmetry in nuclei and beyond
doi: 10.1016/j.nuclphysa.2005.02.012
2005IA05 Phys.Rev.Lett. 95, 052503 (2005) Dynamic Supersymmetries of Differential Equations with Applications to Nuclear Spectroscopy
doi: 10.1103/PhysRevLett.95.052503
2004BI09 Phys.Rev. C 69, 068201 (2004) Reanalysis of the nucleon spacelike and timelike electromagnetic form factors in a two-component model NUCLEAR STRUCTURE 1n, 1H; analyzed electromagnetic form factors. Two-component model.
doi: 10.1103/PhysRevC.69.068201
2004CA48 Phys.Rev.Lett. 93, 242502 (2004) Phase Structure of the two-Fluid Proton-Neutron System
doi: 10.1103/PhysRevLett.93.242502
2004IA03 Eur.Phys.J. A 19, Supplement 1, 29 (2004) Structure of the nucleon from electromagnetic form factors NUCLEAR STRUCTURE 1n, 1H; analyzed form factor data, symmetry effects.
doi: 10.1140/epjad/s2004-03-005-1
2004IA05 Eur.Phys.J. A 20, 1 (2004) Symmetry in physics: On the occasion of receiving the 2002 Lise Meitner medal
doi: 10.1140/epja/i2003-10193-0
2004IA06 Phys.Rev. C 69, 055204 (2004) Structure of the nucleon from electromagnetic timelike form factors NUCLEAR STRUCTURE 1n, 1H; analyzed timelike and spacelike electromagnetic form factors.
doi: 10.1103/PhysRevC.69.055204
2004IA07 Phys.Rev.Lett. 92, 212501 (2004) Quantum Phase Transitions in Mesoscopic Systems NUCLEAR STRUCTURE 148,150,152,154Sm, 152,154,156,158,160Gd; analyzed transitions B(E2), isomer shifts, phase transition features.
doi: 10.1103/PhysRevLett.92.212501
2004IA09 Fizika(Zagreb) B 13, 13 (2004) Structure of the nucleon from electromagnetic form factors NUCLEAR STRUCTURE 1n, 1H; analyzed electromagnetic form factor data; deduced structure features.
2003IA03 Phys.Rev.Lett. 91, 132502 (2003) Phase Transitions in Angle Variables NUCLEAR STRUCTURE 166,168Er, 164Dy; analyzed one- and two-phonon vibrational states features, possible phase transitions in angle variables. Interacting boson model.
doi: 10.1103/PhysRevLett.91.132502
2001IA01 Phys.Rev.Lett. 87, 052502 (2001) Analytic Description of Critical Point Nuclei in a Spherical-Axially Deformed Shape Phase Transition
doi: 10.1103/PhysRevLett.87.052502
2000AR21 Ann.Phys.(New York) 281, 2 (2000) Interacting Boson Model of Collective States I. The Vibrational Limit NUCLEAR STRUCTURE 102Rh, 110Cd, 188Pt, 100Pd, 150Sm, 152Gd, 156Er; calculated levels. Interacting boson model. Reprint of earlier article.
doi: 10.1006/aphy.2000.6007
2000BI13 Phys.Rev. C61, 067305 (2000) Cluster States in Nuclei as Representations of a U(ν + 1) Group NUCLEAR STRUCTURE 12C; calculated levels, J, π. Cluster model.
doi: 10.1103/PhysRevC.61.067305
2000IA03 Phys.Rev.Lett. 85, 3580 (2000) Dynamic Symmetries at the Critical Point
doi: 10.1103/PhysRevLett.85.3580
1999GE20 Prog.Theor.Phys.(Kyoto) 101, 1261 (1999) A.Gelberg, F.Iachello, T.Otsuka, R.V.Jolos Generation of Irreducible Representations in the 0(6) Limit of the IBM
doi: 10.1143/PTP.101.1261
1999IA01 J.Phys.(London) G25, 655 (1999) Dynamic Symmetries in Nuclei
doi: 10.1088/0954-3899/25/4/014
1999TO03 Phys.Rev. C59, 1526 (1999) E.Tomasi-Gustafsson, M.P.Rekalo, R.Bijker, A.Leviatan, F.Iachello Sensitivity of Tensor Analyzing Power in the Process d + p → d + X to the Longitudinal Isoscalar Form Factor of the Roper Resonance Electroexcitation NUCLEAR REACTIONS 1H(polarized d, d'X), E at 3.7-9 GeV/c; calculated tensor analyzing power T20(q); deduced resonance contributions. Algebraic collective model.
doi: 10.1103/PhysRevC.59.1526
1998SA11 Eur.Phys.J. A 1, 307 (1998) E.Santopinto, F.Iachello, M.M.Giannini Nucleon Form Factors in a Simple Three-Body Quark Model
doi: 10.1007/s100500050065
1997SA49 Nucl.Phys. A623, 100c (1997) E.Santopinto, F.Iachello, M.M.Giannini Exactly Solvable Models of Baryon Spectroscopy
doi: 10.1016/S0375-9474(97)00427-2
1996BI14 Phys.Rev. C54, 1935 (1996) R.Bijker, F.Iachello, A.Leviatan Electromagnetic Form Factors in a Collective Model of the Nucleon NUCLEAR STRUCTURE 1H, 1n; analyzed electromagnetic form factors, helicity amplitudes data. Collective baryons model, algebraic approach to hadron structure.
doi: 10.1103/PhysRevC.54.1935
1996CA10 Phys.Rev. C53, 1618 (1996) S.Cacciamani, G.Bonsignori, F.Iachello, D.Vretenar Broken Pairs in the Interacting Boson Model: Projection of spurious states NUCLEAR STRUCTURE 116Sn, 82Sr; calculated levels, B(λ). Interacting boson model, broken pairs, spurious states projection.
doi: 10.1103/PhysRevC.53.1618
1994IA01 Nucl.Phys. A570, 145c (1994) Superconductivity in Finite Fermi Systems NUCLEAR STRUCTURE N=51-81; compiled, reviewed observed, ideal spectra in Sn isotopes; deduced interacting boson model of metal clusters possibility.
doi: 10.1016/0375-9474(94)90278-X
1993IA01 Nucl.Phys. A560, 23 (1993) Algebraic Methods in Quantum Mechanics with Applications to Nuclear and Molecular Structure NUCLEAR STRUCTURE 156Gd; analyzed levels. 134Ba; analyzed E2 γ-transition branching ratios. Algebraic methods.
doi: 10.1016/0375-9474(93)90080-H
1991IA01 Phys.Rev. C43, R945 (1991) Physics of High-Spin States in Nuclei NUCLEAR STRUCTURE 194Hg; calculated yrast levels. Interacting boson model, two broken pairs.
doi: 10.1103/PhysRevC.43.R945
1991IA02 Nucl.Phys. A522, 83c (1991) Physics of High-Spin States in the Interacting Boson Model NUCLEAR STRUCTURE 192Hg; analyzed data; deduced superdeformed band features. Other nuclei discussed. Interacting boson model.
doi: 10.1016/0375-9474(91)90052-8
1990IA01 Nucl.Phys. A507, 43c (1990) The Shell Model and the Interacting Boson Model NUCLEAR STRUCTURE A=18-140; compiled calculated level spectra, B(λ). Interacting boson, shell model relationships.
doi: 10.1016/0375-9474(90)90567-6
1990IA02 Fizika(Zagreb) 22, 57 (1990) Generalized Alaga Rules NUCLEAR STRUCTURE 124,126,128,130Xe; calculated B(λ) ratios; deduced dynamical supersymmetry, symmetry connection to generalized Alaga rules. 197Au; calculated B(λ); deduced dynamical supersymmetry, symmetry connection to generalized Alaga rules.
1989AL21 Nucl.Phys. A501, 585 (1989) Algebracic Approach to Heavy-Ion Reactions NUCLEAR REACTIONS 24Mg(16O, 16O), (16O, 16O'), (16O, 12C), E(cm)=27.8 MeV; calculated σ(θ). Algebraic approach.
doi: 10.1016/0375-9474(89)90150-4
1989DE07 Phys.Lett. 218B, 399 (1989) Beta Decay of Odd-A Nuclei in the Interacting Boson-Fermion Model NUCLEAR STRUCTURE 118,120,122,124,126,128,130,132I; calculated Gamow-Teller transition matrix elements. Interacting boson-fermion model.
doi: 10.1016/0370-2693(89)91434-2
1989IA01 Ann.Phys.(New York) 192, 133 (1989) The Role of Dynamic Symmetries and Supersymmetries in Nuclear Physics NUCLEAR STRUCTURE 110Cd, 156Gd, 196Pt; calculated levels; deduced dynamical symmetry role. 190Os, 191Ir; calculated levels; deduced dynamical supersymmetry role. Dynamic symmetries, supersymmetries.
doi: 10.1016/0003-4916(89)90122-X
1988AL06 Phys.Lett. 201B, 183 (1988) Y.Alhassid, F.Iachello, B.Shao A Study of Heavy-Ion Reactions in the Algebraic Scattering Theory NUCLEAR REACTIONS 24Mg(16O, 16O), (16O, 16O'), 28Si(12C, 12C), (12C, 12C'), E(cm)=27.8 MeV; calculated σ(θ). Algebraic scattering theory.
doi: 10.1016/0370-2693(88)90208-0
1988KU15 Phys.Lett. 209B, 420 (1988) A Study of Collective Octupole States in Barium in the Interacting Boson Model NUCLEAR STRUCTURE 140,142,144,146,148Ba; calculated levels, B(λ) ratios. Interacting spdf boson model.
doi: 10.1016/0370-2693(88)91166-5
1987EN05 Nucl.Phys. A472, 61 (1987) Interacting Boson Model of Collective Octupole States (I). The Rotational Limit NUCLEAR STRUCTURE 220,222,224,226,218Ra; calculated levels, B(λ) ratios. Interacting boson model.
doi: 10.1016/0375-9474(87)90220-X
1985AL25 Phys.Lett. 164B, 241 (1985) C.E.Alonso, J.M.Arias, F.Iachello Nuclear Structure Information Obtained from Charge Radii NUCLEAR STRUCTURE 126,128,129,130,131,132,133,134Xe, 121,123,125,127,129,131,133,135Cs; analyzed rms charge radii data. Interacting boson model.
doi: 10.1016/0370-2693(85)90317-X
1985BI02 Ann.Phys.(New York) 161, 360 (1985) Interacting Boson-Fermion Model of Collective States. III. The SO(6)(x)U(2) Limit NUCLEAR STRUCTURE 195Pt; calculated levels, B(E2), one-nucleon transfer S. Interacting boson-fermion model, SO(6)xU(2) limit.
doi: 10.1016/0003-4916(85)90085-5
1985IA02 Phys.Lett. 160B, 1 (1985) Local Versus Global Isospin Symmetry in Nuclei NUCLEAR STRUCTURE 18O, 220Ra; calculated dipole moments, B(E1). 150Nd; calculated dipole moments, B(E1), E1 strength distribution; deduced isospin, symmetry connection. Octupole, clustering deformations.
doi: 10.1016/0370-2693(85)91455-8
1985MA07 Phys.Lett. 152B, 17 (1985) G.Maino, A.Ventura, L.Zuffi, F.Iachello Photon Scattering in the Interacting Boson Model NUCLEAR REACTIONS 232Th(γ, X), E=9-17 MeV; 238U(γ, X), E=8-20 MeV; calculated photoabsorption σ(E). Interacting boson model.
doi: 10.1016/0370-2693(85)91130-X
1984AL19 Phys.Lett. 144B, 141 (1984) C.E.Alonso, J.M.Arias, R.Bijker, F.Iachello A Calculation of Low-Lying Collective States in Odd-Even Nuclei NUCLEAR STRUCTURE 109,111,113,115,117,119,121,123,125,127,129Xe; 111,113,115,117,119,121,123,125,127,129,131,133Cs; calculated negative parity states.
doi: 10.1016/0370-2693(84)91790-8
1984MA55 Phys.Rev. C30, 2101 (1984) G.Maino, A.Ventura, L.Zuffi, F.Iachello Properties of Giant Resonances in the Interacting Boson Model NUCLEAR STRUCTURE 144,146,148,150Nd, 148,150,152,154Sm; calculated collective GDR, E1 transition strength distribution. Interacting boson model. NUCLEAR REACTIONS 144,146,148,150Nd, 148,150,152,154Sm(γ, X), E=8-20 MeV; calculated photoabsorption σ(E); deduced model parameters. Interacting boson model.
doi: 10.1103/PhysRevC.30.2101
1983BA16 Phys.Rev. C27, 1761 (1983) A.B.Balantekin, I.Bars, R.Bijker, F.Iachello New Class of Supersymmetry in Nuclei NUCLEAR STRUCTURE 195Pt; calculated levels; deduced new supersymmetry classification.
doi: 10.1103/PhysRevC.27.1761
1983DA28 Phys.Lett. 131B, 281 (1983) Alpha-Clustering in Heavy Nuclei NUCLEAR STRUCTURE 216,218,220,222,224,226,228,230Ra, 218,220,222,224,226,228,230,232Th; calculated levels. 224Ra; calculated configuration mixing. Algebraic approach, α-clustering.
doi: 10.1016/0370-2693(83)90498-7
1983IA01 Nucl.Phys. A396, 233c (1983) Algebraic Approach to Nuclear Structure NUCLEAR STRUCTURE 20Ne, 220,222,224,226,228Ra, 224,226,228,230,232,234Th, 8Be; calculated levels. Cluster model, algebraic approach.
doi: 10.1016/0375-9474(83)90022-2
1981BA24 Phys.Rev.Lett. 47, 19 (1981) A.B.Balantekin, I.Bars, F.Iachello U(6/4) Dynamical Supersymmetry in Nuclei NUCLEAR STRUCTURE 190Os, 191Ir; calculated levels; deduced supersymmetry scheme. Group, U(6/4).
doi: 10.1103/PhysRevLett.47.19
1981BA47 Nucl.Phys. A370, 284 (1981) A.B.Balantekin, I.Bars, F.Iachello U(6/4) Supersymmetry in Nuclei NUCLEAR STRUCTURE 196Pt, 191,193Ir, 190,192Os; calculated levels; deduced supersymmetry scheme. 198,196Hg, 192,194,196Pt, 191,193Ir, 190,192Os; calculated B(E2); deduced supersymmetry scheme. Group, U(6/4).
doi: 10.1016/0375-9474(81)90078-6
1981IA01 Ann.Phys.(New York) 136, 19 (1981) Interacting Boson-Fermion Model of Collective States 1. The Spin (6) Limit NUCLEAR STRUCTURE 191,193Ir; calculated levels, B(λ), quadrupole moments, μ. Interacting boson, fermion model, spin (6) limit.
doi: 10.1016/0003-4916(81)90085-3
1980DI08 Phys.Rev.Lett. 44, 1747 (1980) A.E.L.Dieperink, O.Scholten, F.Iachello Classical Limit of the Interacting-Boson Model NUCLEAR STRUCTURE Nd, Sm, Gd, Os, Pt; calculated two-neutron separation energies, equilibrium shapes; deduced nature of shape transitions. Interacting boson model.
doi: 10.1103/PhysRevLett.44.1747
1980IA01 Phys.Rev.Lett. 44, 772 (1980) Dynamical Supersymmetries in Nuclei NUCLEAR STRUCTURE 192Pt, 191Ir; calculated levels; deduced supersymmetry structure of levels.
doi: 10.1103/PhysRevLett.44.772
1980IA02 Phys.Lett. 91B, 189 (1980) New Coupling Scheme in the Interacting Boson-Fermion Model: O(6) Spectra in Odd-A Nuclei NUCLEAR STRUCTURE 191Au; calculated levels. Interacting boson-fermion model.
doi: 10.1016/0370-2693(80)90427-X
1979IA01 Phys.Rev.Lett. 43, 679 (1979) Interacting Boson-Fermium Model of Collective States in Odd-A Nuclei NUCLEAR STRUCTURE 155Eu; calculated spectra. Interacting boson-fermion model.
doi: 10.1103/PhysRevLett.43.679
1979IA02 Phys.Lett. 89B, 1 (1979) F.Iachello, G.Puddu, O.Scholten, A.Arima, T.Otsuka A Calculation of Low-Lying Collective States in Even-Even Nuclei NUCLEAR STRUCTURE 108,110,112,114,116,118,120,122,124,126,128,130,132Xe, 110,112,114,116,118,120,122,124,126,128,130,132,134Ba, 112,114,116,118,120,122,124,126,128,130,132,134,136Ce; calculated collective states. Proton-neutron interacting boson model.
doi: 10.1016/0370-2693(79)90061-3
1978DI07 Phys.Lett. 76B, 135 (1978) A.E.L.Dieperink, F.Iachello, A.Rinat, C.Creswell Electron Scattering in the Interacting Boson Model NUCLEAR STRUCTURE 150Nd, 150,152,154Sm; calculated B(E2). Interacting boson model.
doi: 10.1016/0370-2693(78)90259-9
1976AR09 Ann.Phys. (New York) 99, 253 (1976) Interacting Boson Model of Collective States. I. The Vibrational Limit NUCLEAR STRUCTURE 102Ru, 110Cd, 188Pt, 100Pd, 150Sm, 152Gd, 156Er; calculated levels. Interacting boson model.
doi: 10.1016/0003-4916(76)90097-X
1975AR09 Phys.Lett. 57B, 39 (1975) Elementary Excitations in Vibrational Nuclei NUCLEAR STRUCTURE 152Gd; calculated levels.
doi: 10.1016/0370-2693(75)90238-5
1974IA02 Phys.Lett. 48B, 81 (1974) Effects of Intermediate Channels in Isospin Forbidden Reactions NUCLEAR REACTIONS 12C(d, d'); calculated intermediate channels contribution to isospin forbidden reactions.
doi: 10.1016/0370-2693(74)90647-9
1974IA03 Nucl.Phys. A228, 356 (1974) Effects of Proton Pair Vibrations in the Low-Lying Spectrum of Closed-Shell Nuclei: Structure of 48Ca NUCLEAR STRUCTURE 48Ca; calculated levels.
doi: 10.1016/0375-9474(74)90439-4
1974IA04 Phys.Lett. 53B, 309 (1974) Boson Symmetries in Vibrational Nuclei NUCLEAR STRUCTURE 100Pd; calculated levels.
doi: 10.1016/0370-2693(74)90389-X
1974SM05 Phys.Lett. 53B, 337 (1974) J.W.Smits, F.Iachello, R.H.Siemssen, A.Van der Woude Coherence Effects in the (p, α) Reaction NUCLEAR REACTIONS 118Sn(p, α), E=22 MeV; measured σ(Eα, θ). 115Sn levels deduced S.
doi: 10.1016/0370-2693(74)90396-7
1974VA17 Phys.Rev.Lett. 33, 712 (1974) S.Y.van der Werf, B.R.Kooistra, W.H.A.Hesselink, F.Iachello, L.W.Put, R.H.Siemssen Deeply Bound Hole States as a Giant-Resonance-Like Phenomenon NUCLEAR REACTIONS 112,116,118,120,122,124Sn(d, t), E=50 MeV; measured σ(Et, θ). 115Sn resonances deduced L. 111,115,117,119,121,123Sn deduced resonance structure.
doi: 10.1103/PhysRevLett.33.712
1973FE04 Phys.Lett. 45B, 7 (1973) The Interacting Boson Model Structure of 16O NUCLEAR STRUCTURE 16O; calculated levels, α-width, B(E2), interacting Boson model.
doi: 10.1016/0370-2693(73)90239-6
1971IA01 Phys.Lett. 35B, 205 (1971) Meson Finite Size Effects in Mesonic Atoms ATOMIC PHYSICS, Mesic-Atoms 206Pb; calculated π polarization, higher-order corrections to transitions.
doi: 10.1016/0370-2693(71)90175-4
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