NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = J.P.Elliott Found 35 matches. 1999EL03 J.Phys.(London) G25, 577 (1999) Recollections of the Introduction of SU(3) to Nuclear Theory
doi: 10.1088/0954-3899/25/4/002
1999EL04 J.Phys.(London) G25, 667 (1999) J.P.Elliott, J.A.Evans, P.Halse Mappings from Shell-Model SU(3) to Boson SU(3)
doi: 10.1088/0954-3899/25/4/016
1999EL09 J.Phys.(London) G25, 2071 (1999) A Direct Mapping from Shell Model SU(3) to Boson SU(3)
doi: 10.1088/0954-3899/25/10/307
1997EV05 Nucl.Phys. A627, 71 (1997) J.A.Evans, V.S.Lac, J.P.Elliott A New Method for IBM3 Calculations
doi: 10.1016/S0375-9474(97)00590-3
1997LA12 Phys.Lett. 394B, 231 (1997) V.S.Lac, J.P.Elliott, J.A.Evans On the Validity of the O(18) Coupling Scheme in N ∼ Z Nuclei NUCLEAR STRUCTURE 62,64Zn, 64,66Ge, 68Se; calculated 0+, 2+, 3+, 4+ states, wave functions; deduced O(18) coupling scheme validity related features.
doi: 10.1016/S0370-2693(97)00027-0
1996EL02 Nucl.Phys. A597, 341 (1996) J.P.Elliott, J.A.Evans, V.S.Lac Electromagnetic Operators in IBM-3 and Their Dependence on the Boson Number and Isospin
doi: 10.1016/0375-9474(95)00475-0
1996EL10 Nucl.Phys. A609, 1 (1996) J.P.Elliott, J.A.Evans, V.S.Lac, G.L.Long An IBM-3 Analysis of the Nuclei Just Beyond the Magic Numbers N = Z = 28 NUCLEAR STRUCTURE 58,60,62,64Ni, 60,62,64,66Zn, 64,66,68Ge, 68Se; calculated binding energies, level spectra, B(λ). Isospin-invariant form of IBM-3.
doi: 10.1016/S0375-9474(96)00292-8
1995EV02 Nucl.Phys. A593, 85 (1995) J.A.Evans, J.P.Elliott, V.S.Lac, G.L.Long An IBM-3 Hamiltonian from a Multi-j-Shell Model
doi: 10.1016/0375-9474(95)00326-V
1995LA06 Nucl.Phys. A587, 101 (1995) V.S.Lac, J.P.Elliott, J.A.Evans, G.L.Long A Comparison of the IBM-1 Projections from IBM-2 and IBM-3
doi: 10.1016/0375-9474(94)00811-Z
1989AB13 Nucl.Phys. A503, 452 (1989) M.Abdelaziz, J.P.Elliott, M.J.Thompson, J.A.Evans On the Role of Isoscalar Bosons in Lighter Nuclei NUCLEAR STRUCTURE 46V, 48Cr, 46,44Ti, 44Sc; calculated levels, B(λ). 44Cr; calculated β-decay log ft. Shell model wave functions, boson analysis.
doi: 10.1016/0375-9474(89)90244-3
1989TH05 Nucl.Phys. A504, 436 (1989) M.J.Thompson, J.P.Elliott, J.A.Evans A Microscopic IBM2 Hamiltonian for Particle-Hole Systems NUCLEAR STRUCTURE 46Ti, 48Cr, 89,90Zr; calculated levels. Microscopic interacting boson model.
doi: 10.1016/0375-9474(89)90550-2
1988AB02 J.Phys.(London) G14, 219 (1988) M.Abdelaziz, M.J.Thompson, J.P.Elliott, J.A.Evans Shell Model and IBM Descriptions of Mixed Symmetry or Isovector M1 Transitions in the Titanium Isotopes NUCLEAR STRUCTURE 44,46,48Ti, 48Cr; calculated levels, B(M1). Shell, interacting boson models.
doi: 10.1088/0305-4616/14/2/014
1988EV01 Nucl.Phys. A489, 269 (1988) J.A.Evans, P.Van Isacker, J.P.Elliott A Test of the Interacting Boson-Fermion Model in a Single j-Shell of Neutrons and Protons NUCLEAR STRUCTURE 45Ti, 45Sc, 47V; calculated levels. Shell model.
doi: 10.1016/0375-9474(88)90153-4
1987AB11 Phys.Lett. 197B, 505 (1987) The β-Decay of 48Cr and Low Energy Collective M1 Transitions NUCLEAR STRUCTURE 48Cr; analyzed β-decay T1/2 data. 44,46,48Ti, 48Cr deduced spin contribution to B(M1). Other data input.
doi: 10.1016/0370-2693(87)91043-4
1987TH05 Phys.Lett. 195B, 511 (1987) M.J.Thompson, J.P.Elliott, J.A.Evans A Microscopically Determined IBM 3 Hamiltonian NUCLEAR STRUCTURE 46Ti; calculated T = 1 spectrum. Interacting boson model.
doi: 10.1016/0370-2693(87)91563-2
1987VA25 Phys.Rev. C36, 1229 (1987) P.Van Isacker, J.P.Elliott, D.D.Warner Rotational versus Pseudo-L Symmetries in the Interacting Boson-Fermion-Model Description of Deformed Nuclei NUCLEAR STRUCTURE 183,185,187W; calculated levels, single particle transfer strengths. Interacting boson-fermion model, SU(3) symmetry.
doi: 10.1103/PhysRevC.36.1229
1986EI01 Phys.Lett. 166B, 267 (1986) S.A.A.Eid, W.D.Hamilton, J.P.Elliott A Shared Mixed-Symmetry State in 56Fe RADIOACTIVITY 56Mn(β-); measured γ(θ), oriented nuclei. 56Fe deduced 2+ level decay characteristics.
doi: 10.1016/0370-2693(86)90795-1
1986PA01 Nucl.Phys. A448, 381 (1986) The Effects of Core Polarisation on IBM Calculations NUCLEAR REACTIONS 20Ne, 24Mg(e, e'), E not given; calculated form factors. Interacting boson model, core polarization. NUCLEAR STRUCTURE 22,24Ne, 26Mg; calculated levels. 24Mg; calculated transition density, levels. Interacting boson model, core polarization.
doi: 10.1016/0375-9474(86)90334-9
1985EL12 Nucl.Phys. A437, 208 (1985) J.P.Elliott, J.A.Evans, E.E.Maqueda α-Transfer and a Tetrahedral Shape for 16O NUCLEAR STRUCTURE 16O; calculated density contours. Shell model, tetrahedral perturbation, α-clustering. NUCLEAR REACTIONS 12C(6Li, d), E=42 MeV; calculated σ(θ); deduced optical model parameters, reaction mechanism. 16O levels deduced σ enhancement factors, rotational band structure. Shell model, tetrahedral perturbation, α-clustering.
doi: 10.1016/0375-9474(85)90233-7
1985EV02 Nucl.Phys. A435, 317 (1985) J.A.Evans, J.P.Elliott, S.Szpikowski An IBM Analysis of a Single j-Shell of Neutrons and Protons NUCLEAR STRUCTURE 44,46Ti, 44Sc, 44Ca; calculated level energies; deduced shell model analog of U(6), U(5) boson labels.
doi: 10.1016/0375-9474(85)90467-1
1985PA26 J.Phys.(London) G11, L251 (1985) P.Park, A.R.H.Subber, W.D.Hamilton, J.P.Elliott, K.Kumar A Study of the γ-Unstable Nucleus 124Te NUCLEAR STRUCTURE 124Te; calculated potential energy, levels, B(λ). Dynamic deformation model.
doi: 10.1088/0305-4616/11/12/005
1984HA14 Nucl.Phys. A417, 301 (1984) P.Halse, J.P.Elliott, J.A.Evans An Application of the Interacting Boson Model to the First Half of the sd Shell (1). Even-Even Nuclei NUCLEAR STRUCTURE 20,22,24Ne, 20,22O, 20,24,26,28Mg, 28Si; calculated levels, B(E2), binding energies relative to 16O. Interacting boson model.
doi: 10.1016/0375-9474(84)90510-4
1984HA49 Phys.Rev.Lett. 53, 2469 (1984) W.D.Hamilton, A.Irback, J.P.Elliott Mixed-Symmetry Interacting-Boson-Model States in the Nuclei 140Ba, 142Ce, and 144Nd with N = 84 NUCLEAR STRUCTURE 140Ba, 140Ce, 144Nd; analyzed 2+ level γ-decay data; deduced mixed symmetry characteristics. Interacting boson model, U(5) limit.
doi: 10.1103/PhysRevLett.53.2469
1982HA19 Nucl.Phys. A378, 461 (1982) K.Halkia, N.I.Kassis, E.A.Sanderson, J.P.Elliott Effective Interactions and the 4p-4h States in 16O NUCLEAR STRUCTURE 16O; calculated levels, deformation. Hartree-Fock method, four-particle four-hole configuration, density dependent effective interaction.
doi: 10.1016/0375-9474(82)90460-2
1981EL01 Phys.Lett. B97, 169 (1980 An Isospin Invariant Form of the Interacting Boson Model NUCLEAR STRUCTURE 18,20O, 20Ne, 20F; calculated levels. Isospin invariant boson model.
doi: 10.1016/0370-2693(80)90573-0
1979EL04 Nucl.Phys. A324, 12 (1979) The Use of an Angular Momentum Constraint in Calculating Rotational Spectra NUCLEAR STRUCTURE 8Be, 20Ne; calculated spectra. Hartree-Fock method, constraint on square of angular momentum.
doi: 10.1016/0375-9474(79)90073-3
1978HA49 Fizika, Suppl. 10, 39 (1978) K.Halkia, J.P.Elliott, E.A.Sanderson Hartree-Fock Calculations in 16O Using a Cartesian Basis NUCLEAR STRUCTURE 16O; calculated levels, binding energies. Hartree-Fock method, cartesian basis.
1977TR01 Nucl.Phys. A278, 78 (1977) R.K.Tripathi, E.A.Sanderson, J.P.Elliott Third-Order Contributions to the Binding Energy of Oxygen NUCLEAR STRUCTURE 16O; calculated third-order contribution to binding energy.
doi: 10.1016/0375-9474(77)90185-3
1975DI04 Nucl.Phys. A244, 301 (1975) H.Dirim, J.P.Elliott, J.A.Evans The Effective Hamiltonian and Spectra of the 0π Shell NUCLEAR STRUCTURE 6,7Li, 10B, 14N; calculated levels. Modified Sussex matrix elements.
doi: 10.1016/0375-9474(75)90060-3
1974SA05 Nucl.Phys. A219, 190 (1974) E.A.Sanderson, J.P.Elliott, H.A.Mavromatis, B.Singh Second Order Binding Energies and Spectra with an Interaction Matrix Deduced from Phase Shifts NUCLEAR STRUCTURE 4He, 15,16,17O, 39,40,41Ca; calculated binding energies. 18O, 18F calculated levels.
doi: 10.1016/0375-9474(74)90091-8
1972NI15 Nucl.Phys. A198, 1 (1972) Some Comments on Perturbation Theory
doi: 10.1016/0375-9474(72)90767-1
1969DE16 Nucl.Phys. A134, 385 (1969) J.Dey, J.P.Elliott, A.D.Jackson, H.A.Mavromatis, E.A.Sanderson, B.Singh First-Order Binding Energies and Spectra with a Potential Matrix Deduced from Phase Shifts NUCLEAR STRUCTURE 15,17O, 39,41Ca, 91Zr, 207,209Pb; calculated levels, binding energies.
doi: 10.1016/0375-9474(69)91062-8
1967BO09 Nucl.Phys. A97, 113 (1967) M.C.Bouten, J.P.Elliott, J.A.Pullen Intermediate Coupling in the Nuclear ds-shell
doi: 10.1016/0375-9474(67)90774-9
1967EL03 Phys.Letters 24B, 358 (1967) J.P.Elliott, H.A.Mavromatis, E.A.Sanderson Direct Calculation of Nuclear Structure from the Two-Nucleon Phase Shifts
doi: 10.1016/0370-2693(67)90288-2
1963EL01 Proc.Roy.Soc.(London) 272A, 557 (1963) Collective Motion in the Nuclear Shell Model. III. The Calculation of Spectra NUCLEAR STRUCTURE 24Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1098/rspa.1963.0071
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