NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Svenne Found 52 matches. 2019FR03 Phys.Rev. C 100, 024609 (2019) P.R.Fraser, K.Amos, L.Canton, S.Karataglidis, D.van der Knijff, J.P.Svenne Mass-15 nuclei and predicting narrow states beyond the proton drip line NUCLEAR STRUCTURE 15C, 15N, 15O, 15F; calculated levels, J, π and widths using multichannel algebraic scattering (MCAS) technique, and n+14O or p+14C and p+14O or n+14C mirror systems. Comparison with experimental data. NUCLEAR REACTIONS 1H(14O, 15F), E=E=95 MeV/nucleon; calculated cross sections for population of levels in 15F using multichannel algebraic scattering (MCAS) technique, and using the vibrational model for the interaction potential for p+14O cluster. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.024609
2017AM02 Eur.Phys.J. A 53, 72 (2017) K.Amos, L.Canton, P.R.Fraser, S.Karataglidis, J.P.Svenne, D.van der Knijff A multi-channel model for an α plus 6He nucleus cluster NUCLEAR REACTIONS 4He(6He, 6He'), E=2-6 MeV(10Be E*=9.4-13.4 MeV); calculated σ(θ). Compared with data. NUCLEAR STRUCTURE 10Be; calculated levels, J, πi, charge distribution using three- and five-state MCAS (Multi-Channel Algebraic Scattering). Compared with data.
doi: 10.1140/epja/i2017-12270-1
2017SV01 Phys.Rev. C 95, 034305 (2017) J.P.Svenne, L.Canton, K.Amos, P.R.Fraser, S.Karataglidis, G.Pisent, D.van der Knijff Very low-energy nucleon-16O coupled-channel scattering: Results with a phenomenological vibrational model NUCLEAR STRUCTURE 17O, 17F; calculated levels, J, π, widths. 16O; calculated B(E2) for the first 2+ and B(E3) for the first 3- state, ρ2(E0) for the first excited 0+ state. Multichannel algebraic scattering method (MCAS)for bound states and resonances. Comparison with experimental data. NUCLEAR REACTIONS 16O(n, X), E=0.001-8.5 MeV; calculated total σ(E). 16O(p, X), E<4.5 MeV; calculated differential σ(E, θ). Multichannel algebraic scattering method (MCAS) for nucleon-16O cluster systems. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.034305
2016FR09 Phys.Rev. C 94, 034603 (2016) P.R.Fraser, K.Massen-Hane, K.Amos, I.Bray, L.Canton, R.Fossion, A.S.Kadyrov, S.Karataglidis, J.P.Svenne, D.van der Knijff Importance of resonance widths in low-energy scattering of weakly bound light-mass nuclei NUCLEAR STRUCTURE 9Be; calculated levels, resonances J, π, widths of a compound nucleus with 8Be+n cluster by solving the Lippmann-Schwinger equations in momentum space. Comparison with multichannel algebraic scattering (MCAS) calculations with target states. NUCLEAR REACTIONS 8Be(n, n), E<5.5 MeV; 12C(n, n), (n, X), E<6.5 MeV; calculated elastic and reaction σ(E) coupled to first 0+, 2+ and 4+ states in 8Be, reaction σ with particle emission widths of 12C coupled to g.s., first 2+ and first excited 0+ states in 12C; deduced effect of particle-emitting resonances on the scattering cross section. Method involved choosing an appropriate target-state resonance shape, modifying a Lorentzian by use of widths dependent on projectile energy, with a correction to target-state centroid energy.
doi: 10.1103/PhysRevC.94.034603
2015FR04 Eur.Phys.J. A 51, 110 (2015) P.R.Fraser, K.Amos, L.Canton, S.Karataglidis, D.van der Knijff, J.P.Svenne A collective coupled-channel model and mirror state energy displacements NUCLEAR STRUCTURE 12C; calculated charge distribution, radius; deduced interaction parameters. 13,15C, 13,15,16N, 15,16O, 15F; calculated energy levels, J, π; deduced interaction parameters. MCAS (multi-channel algebraic scattering) method; compared to data. NUCLEAR REACTIONS 1H(14O, 14O'), E(cm)=0.3-9 MeV; calculated σ(θ) using MCAS (multi-channel algebraic scattering) method; compared to data.
doi: 10.1140/epja/i2015-15110-4
2014FR08 Phys.Rev. C 90, 024616 (2014) P.R.Fraser, L.Canton, K.Amos, S.Karataglidis, J.P.Svenne, D.van der Knijff Coupling to two target-state bands in the study of the n+22Ne system at low energy NUCLEAR STRUCTURE 22Ne; calculated low-lying levels, J, π, dominant partition percentages, β2, B(E2) using large-space shell-model. 23Ne; calculated levels, resonances, J, π by coupling to low-lying states in 22Ne using multichannel algebraic scattering (MCAS) formalism for n+22Ne system; comparison with experimental spectrum of 23Ne. NUCLEAR REACTIONS 22Ne(n, n), E<4.5 MeV; calculated elastic σ(E), resonances, J, π using multichannel algebraic scattering (MCAS) formalism. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.024616
2014NA25 Nucl.Data Sheets 119, 98 (2014) N.Nankov, A.J.M.Plompen, S.Kopecky, K.S.Kozier, D.Roubtsov, R.Rao, R.Beyer, E.Grosse, R.Hannaske, A.R.Junghans, R.Massarczyk, R.Schwengner, D.Yakorev, A.Wagner, M.Stanoiu, L.Canton, R.Nolte, S.Rottger, J.Beyer, J.Svenne The Angular Distribution of Neutrons Scattered from Deuterium below 2 MeV NUCLEAR REACTIONS 2H(n, n), E=0.1-2 MeV; Measured En, In(θ=150), In(θ=1650) using nELBE neutron ToF facility; deduced neutron spectra, deuteron counts at forward and backward directions.
doi: 10.1016/j.nds.2014.08.028
2014RO12 Nucl.Data Sheets 118, 414 (2014) D.Roubtsov, K.S.Kozier, J.C.Chow, A.J.M.Plompen, S.Kopecky, J.P.Svenne, L.Canton Reactivity Impact of 2H and 16O Elastic Scattering Nuclear Data on Critical Systems with Heavy Water NUCLEAR REACTIONS 2H, 16O(n, n), E=0.0001 eV-2 MeV; evaluated elastic scattering σ for critical systems with heavy water, influence on reactivity.
doi: 10.1016/j.nds.2014.04.094
2013AM01 Nucl.Phys. A912, 7 (2013) K.Amos, L.Canton, P.R.Fraser, S.Karataglidis, J.P.Svenne, D.van der Knijff Analysis of a coupled-channel continuum approach for spectra of mass-17 compound systems NUCLEAR STRUCTURE 17C, 17Na; calculated levels, J, π, level widths using MCAS (multi-channel algebraic scattering).
doi: 10.1016/j.nuclphysa.2013.05.008
2012AM01 Nucl.Phys. A879, 132 (2012) K.Amos, L.Canton, P.R.Fraser, S.Karataglidis, J.P.Svenne, D.van der Knijff Linking the exotic structure of 17C to its unbound mirror 17Na NUCLEAR STRUCTURE 17C, 17Na; calculated low-lying resonances, deformation using MCAS (multichannel algebraic scattering) method to coupled Lippmann-Schwinger equation in momentum space and CC model of nucleon-nucleus structure; deduced parameters.
doi: 10.1016/j.nuclphysa.2012.01.022
2012AM06 Europhys.Lett. 99, 12001 (2012) K.Amos, D.van der Knijff, L.Canton, P.R.Fraser, S.Karataglidis, J.P.Svenne Linking nuclear masses with nucleon-removal thresholds and the mass of the proton-emitter 17Na NUCLEAR STRUCTURE 6,7Li, 8,9Be, 10,11B, 12,13,17C, 14,15,17N, 16,17O, 17,18,19F, 17,20Ne, 17Na; calculated ground state gap energies, masses, nucleon removal thresholds. Comparison with available data.
doi: 10.1209/0295-5075/99/12001
2011CA10 Phys.Rev. C 83, 047603 (2011) L.Canton, P.R.Fraser, J.P.Svenne, K.Amos, S.Karataglidis, D.van der Knijff Energy-dependent target widths in a coupled-channel scattering study NUCLEAR REACTIONS 8Be(n, n), (n, n'), E=0-6 MeV; calculated σ(E). 9Be; calculated resonances, J, π, width using multichannel algebraic scattering formalism for particle emitting resonances. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.047603
2011ST25 J.Korean Phys.Soc. 59, 1825s (2011) M.Stanoiu, N.Nankov, A.J.M.Plompen, C.Rouki, K.Kozier, R.Rao, D.Roubtsov, J.P.Svenne, L.Canton Neutron-Deuteron Elastic Scattering Measurements
doi: 10.3938/jkps.59.1825
2010CA20 Int.J.Mod.Phys. E19, 1435 (2010) L.Canton, K.Amos, S.Karataglidis, J.P.Svenne Coupled-channel calculation of bound and resonant spectra of 9ΛBe and 13ΛC hypernuclei NUCLEAR STRUCTURE 9Be, 13C; analyzed hypernucleus spectra; deduced splitting of levels, spin-orbit, spin-spin, low-lying resonance states. Multi-channel algebraic scattering (MCAS).
doi: 10.1142/S0218301310015849
2008FR02 Eur.Phys.J. A 35, 69 (2008) P.Fraser, K.Amos, S.Karataglidis, L.Canton, G.Pisent, J.P.Svenne Two causes of nonlocalities in nucleon-nucleus potentials and their effects in nucleon-nucleus scattering NUCLEAR REACTIONS 12C(n, n), (n, n'), E=40.3, 95 MeV; 12C(p, p), (p, p'), E=200 MeV; calculated σ(θ), Ay(θ). 12C(e, e), E not given; calculated longitudinal and transverse form factors. Coupled channel calculations, comparison with data.
doi: 10.1140/epja/i2007-10524-1
2008FR11 Phys.Rev.Lett. 101, 242501 (2008) P.Fraser, K.Amos, L.Canton, G.Pisent, S.Karataglidis, J.P.Svenne, D.van der Knijff Coupled-Channel Evaluations of Cross Sections for Scattering Involving Particle-Unstable Resonances NUCLEAR REACTIONS 12C(n, n'), E < 6 MeV; 8Be(n, n'), E < 4 MeV; calculated cross sections using a multichannnel algebraic scattering approach; 9Be; calculated levels energies, widths. Compared results to available data.
doi: 10.1103/PhysRevLett.101.242501
2008KA39 Nucl.Phys. A813, 235 (2008) S.Karataglidis, K.Amos, P.Fraser, L.Canton, J.P.Svenne Constraints on the spectra of 17, 19C NUCLEAR STRUCTURE 17,19C; analyzed levels, J, radii with shell model and coupled-channel approach, scattering data. NUCLEAR REACTIONS 1H(17C, 17C), (19C, 19C), E=70 MeV/nucleon; analyzed elastic and inelastic σ(θ). 17,19C(p, p'), E=70 MeV; analyzed σ(θ). Microscopic g-folding and distorted wave approximation calculations.
doi: 10.1016/j.nuclphysa.2008.09.007
2008SV02 Few-Body Systems 44, 31 (2008) J.P.Svenne, L.Canton, K.S.Kozier Neutron-deuteron scattering calculation for evaluated neutron data libraries
doi: 10.1007/s00601-008-0250-6
2007CA31 Nucl.Phys. A790, 251c (2007) L.Canton, K.Amos, S.Karataglidis, G.Pisent, J.P.Svenne, D.van der Knijff Particle-unstable and weakly-bound light nuclei with a Sturmian approach that preserves the Pauli principle NUCLEAR REACTIONS 12C(n, n), E≈0.001-5 MeV; calculated σ. Coupled channel calculation. Comparison with data. NUCLEAR STRUCTURE 7He, 7Li, 7Be, 7B, 15C, 15F; calculated levels, J, π, scattering data. Collective-coupling analysis.
doi: 10.1016/j.nuclphysa.2007.03.148
2006CA08 Phys.Rev.Lett. 96, 072502 (2006) L.Canton, G.Pisent, J.P.Svenne, K.Amos, S.Karataglidis Predicting Narrow States in the Spectrum of a Nucleus beyond the Proton Drip Line NUCLEAR STRUCTURE 14,15C, 14O; analyzed levels, scattering data. 15F calculated resonance energies, widths. Multichannel algebraic scattering theory.
doi: 10.1103/PhysRevLett.96.072502
2006CA35 Phys.Rev.C 74, 064605 (2006) L.Canton, G.Pisent, K.Amos, S.Karataglidis, J.P.Svenne, D.van der Knijff Collective-coupling analysis of spectra of mass-7 isobars: 7He, 7Li, 7Be, and 7B NUCLEAR REACTIONS 3H(α, α), E=3-14 MeV; 4He(3He, 3He), E=3-14 MeV; calculated σ(θ). Collective-coupling analysis. NUCLEAR STRUCTURE 7He, 7Li, 7Be, 7B; calculated levels, J, π. Collective-coupling analysis.
doi: 10.1103/PhysRevC.74.064605
2006SV01 Phys.Rev. C 73, 027601 (2006) J.P.Svenne, K.Amos, S.Karataglidis, D.van der Knijff, L.Canton, G.Pisent Low-energy neutron-12C analyzing powers: Results from a multichannel algebraic scattering theory NUCLEAR REACTIONS 12C(polarized n, n), E=1.9-4 MeV; calculated σ(θ), Ay(θ). Multichannel algebraic scattering theory, comparison with data.
doi: 10.1103/PhysRevC.73.027601
2005AM12 Phys.Rev. C 72, 064604 (2005) K.Amos, S.Karataglidis, D.van der Knijff, L.Canton, G.Pisent, J.P.Svenne Comparison between two methods of solution of coupled equations for low-energy scattering NUCLEAR REACTIONS 12C(n, X), E=0.1-4 MeV; analyzed total σ. Comparison of two coupled-channels approaches.
doi: 10.1103/PhysRevC.72.064604
2005CA16 Phys.Rev.Lett. 94, 122503 (2005) L.Canton, G.Pisent, J.P.Svenne, D.van der Knijff, K.Amos, S.Karataglidis Role of the Pauli Principle in Collective-Model Coupled-Channel Calculations NUCLEAR REACTIONS 12C(n, n), E=low; analyzed σ(θ), role of Pauli principle. Multichannel algebraic scattering theory.
doi: 10.1103/PhysRevLett.94.122503
2005PI16 Phys.Rev. C 72, 014601 (2005) G.Pisent, J.P.Svenne, L.Canton, K.Amos, S.Karataglidis, D.van der Knijff Compound and quasicompound states in low-energy scattering of nucleons from 12C NUCLEAR REACTIONS 12C(n, n), E ≈ 0-5 MeV; analyzed elastic σ. 12C(p, p), E ≈ 1-7 MeV; analyzed σ(θ), Ay(θ), σ. 13C, 13N deduced sub-threshold bound state and resonance features. Multichannel algebraic scattering theory.
doi: 10.1103/PhysRevC.72.014601
2003AM08 Nucl.Phys. A728, 65 (2003) K.Amos, L.Canton, G.Pisent, J.P.Svenne, D.van der Knijff An algebraic solution of the multichannel problem applied to low energy nucleon-nucleus scattering NUCLEAR REACTIONS 12C(n, n), E=0-5 MeV; calculated elastic σ, polarization, resonance effects. Sturmian expansions of multichannel interactions. Comparison with data.
doi: 10.1016/j.nuclphysa.2003.08.019
2002ME21 Few-Body Systems 32, 143 (2002) Three-Body Dynamics in One Dimension: A Test Model for the Three-Nucleon System with Irreducible Pionic Diagrams NUCLEAR STRUCTURE A=3; calculated binding energy. Spinless, one-dimensional model.
doi: 10.1007/s00601-002-0114-4
2001CA10 Phys.Rev. C63, 034004 (2001) Practical Approximation Scheme for the Pion Dynamics in the Three-Nucleon System
doi: 10.1103/PhysRevC.63.034004
2001CA19 Nucl.Phys. A684, 417c (2001) L.Canton, G.Pisent, W.Schadow, J.P.Svenne Spin Observables for Pion Production from pd Collisions NUCLEAR REACTIONS 2H(polarized p, π0), E ≈ threshold; calculated Ay(θ). Comparison with data.
doi: 10.1016/S0375-9474(01)00442-0
1998CA09 Phys.Rev. C57, 1588 (1998) L.Canton, G.Cattapan, G.Pisent, W.Schadow, J.P.Svenne Spin Observables for the pd ← → π+t Reaction Around the Δ Resonance NUCLEAR REACTIONS 2H(polarized p, π+), E=350 MeV; calculated σ(θ), A(y0)(θ), T(20)(θ); deduced reaction mechanism, Δ resonance role. Comparison with data.
doi: 10.1103/PhysRevC.57.1588
1996CA26 Can.J.Phys. 74, 209 (1996) L.Canton, G.Cattapan, P.J.Dortmans, G.Pisent, J.P.Svenne A Meson-Exchange Isobar Model for the π+d → pp, pp ← π+d Reaction NUCLEAR REACTIONS 2H(π+, p), E=145 MeV; analyzed σ(θ), polarization observables. Meson-exchange isobar model.
doi: 10.1139/p96-033
1995PI08 Phys.Rev. C51, 3211 (1995) Analysis of Compound and Quasicompound Resonances in a Multichannel, Finite-Rank Model
doi: 10.1103/PhysRevC.51.3211
1993CA29 Phys.Rev. C48, 1562 (1993) L.Canton, J.P.Svenne, G.Cattapan Pion Absorption on 3He. II. Antisymmetrization and Angular Decomposition of the Faddeev-Based Amplitude
doi: 10.1103/PhysRevC.48.1562
1990WA26 Can.J.Phys. 68, 1200 (1990) W.B.Wango, J.Birchall, J.S.C.McKee, J.P.Svenne Evidence for Three-Body Forces in p-d Breakup at 25 MeV ( Question ) NUCLEAR REACTIONS 2H(p, 2p), E=25.05 MeV; measured σ(θ1, θ2, E1) vs arc length following target breakup; deduced three-body force evidence. Faddeev calculations. Collinear geometry.
doi: 10.1139/p90-170
1989AB06 Phys.Rev. D39, 2464 (1989) R.Abegg, D.Bandyopadhyay, J.Birchall, E.B.Cairns, H.Coombes, C.A.Davis, N.E.Davison, P.P.J.Delheij, P.W.Green, L.G.Greeniaus, H.P.Gubler, D.C.Healey, C.Lapointe, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, G.R.Plattner, P.R.Poffenberger, W.D.Ramsay, G.Roy, J.Soukup, J.P.Svenne, R.R.Tkachuk, W.T.H.van Oers, G.D.Wait, Y.P.Zhang Charge-Symmetry Breaking in np Elastic Scattering at 477 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=477 MeV; measured neutron, proton analyzing power difference; deduced isospin violating, charge symmetry breaking effects role.
doi: 10.1103/PhysRevD.39.2464
1989AB11 Phys.Rev. C40, 2406 (1989) R.Abegg, M.Ahmad, D.Bandyopadhyay, J.Birchall, E.B.Cairns, K.Chantziantoniou, H.Coombes, C.A.Davis, N.E.Davison, P.P.J.Delheij, P.W.Green, L.G.Greeniaus, H.P.Gubler, D.C.Healey, C.Lapointe, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, S.A.Page, G.R.Plattner, P.R.Poffenberger, W.D.Ramsay, N.L.Rodning, G.Roy, J.Soukup, J.P.Svenne, R.R.Tkachuk, W.T.H.van Oers, G.D.Wait, J.W.Watson, Y.Ye, Y.P.Zhang np Elastic Scattering Analyzing Power Characteristics at Intermediate Energies NUCLEAR REACTIONS 1H(polarized n, n), E=220-477 MeV; measured polarization observables; deduced analyzing power. Other data input.
doi: 10.1103/PhysRevC.40.2406
1986LE02 Phys.Rev. C33, 417 (1986) Charge-Symmetry Breaking in Neutron-Proton Scattering: Isospin-mixing parameter NUCLEAR REACTIONS 1n(p, p), E=100-400 MeV; calculated isospin mixing parameter; deduced analyzing power difference.
doi: 10.1103/PhysRevC.33.417
1985AB05 Nucl.Instrum.Methods 234, 20 (1985) R.Abegg, J.Birchall, E.Cairns, H.Coombes, C.A.Davis, N.E.Davison, P.W.Green, L.G.Greeniaus, H.P.Gubler, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, G.R.Plattner, P.R.Poffenberger, G.Roy, J.Soukup, J.P.Svenne, R.Tkachuk, W.T.H.van Oers, Y.P.Zhang Detection Equipment For A Test of Charge Symmetry in n-p Elastic Scattering NUCLEAR REACTIONS 1H(polarized n, n), E=150-500 MeV; measured neutron, recoil proton analyzing power, difference.
doi: 10.1016/0168-9002(85)90804-6
1985AB06 Nucl.Instrum.Methods 234, 11 (1985) R.Abegg, J.Birchall, E.Cairns, H.Coombes, C.A.Davis, N.E.Davison, P.W.Green, L.G.Greeniaus, H.P.Gubler, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, G.R.Plattner, P.R.Poffenberger, G.Roy, J.Soukup, J.P.Svenne, R.Tkachuk, W.T.H.Van Oers, Y.P.Zhang The Neutron Beam Facility at TRIUMF NUCLEAR REACTIONS 1H(polarized n, n), E=480 MeV; measured effective analyzing power. High precision experiments.
1985AB18 J.Phys.(Paris), Colloq.C-2, 467 (1985) R.Abegg, J.Birchall, E.Cairns, H.Coombes, C.A.Davis, N.E.Davison, P.P.J.Delheij, P.W.Green, L.G.Greeniaus, H.P.Gubler, D.C.Healey, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, G.R.Plattner, P.R.Poffenberger, G.Roy, J.Soukup, J.P.Svenne, R.Tkachuk, W.T.H.van Oers, G.D.Wait, Y.P.Zhang Test of Charge Symmetry in n-p Elastic Scattering at 480 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=480 MeV; measured neutron, proton analyzing power difference.
1982SV01 Phys.Lett. 119B, 269 (1982) J.P.Svenne, J.Birchall, J.S.C.McKee Possible Evidence for Sensitivity to the Two-Body Tensor Force in the Reaction d + p → p + p + n NUCLEAR REACTIONS 2H(p, 2p), E=25.7 MeV; measured σ(θ1, θ2, E1); deduced breakup sensitivity to two-body tensor force. 1H(polarized d, 2p), E=51.4 MeV; calculated tensor analyzing power vs θ. Three-body model.
doi: 10.1016/0370-2693(82)90667-0
1980AY01 Can.J.Phys. 58, 1026 (1980) Three-Body Calculations of Elastic Scattering and Stripping of Deuterons on 16O NUCLEAR REACTIONS 16O(d, d), (d, n), (d, p), E=20, 45 MeV; 16O(polarized d, d), (polarized d, p), (polarized d, n), E=20 MeV; calculated σ(θ), vector, tensor analyzing power vs θ. Three-body calculations, no Coulomb effects, separable interactions.
doi: 10.1139/p80-141
1980SV01 J.Phys.(London) G6, 465 (1980) A Relation between Average Kinetic Energy and Mean-Square Radius in Nuclei NUCLEAR STRUCTURE 16O, 208Pb; calculated average kinetic energy, single-particle sum rule. Hartree-Fock, Hartree-Fock-Bogoliubov theories.
doi: 10.1088/0305-4616/6/4/015
1979BI07 Phys.Rev. C20, 1585 (1979) J.Birchall, J.P.Svenne, M.S.de Jong, J.S.C.McKee, W.D.Ramsay, M.S.A.L.Al-Ghazi, N.Videla Proton-Deuteron Breakup Cross Sections in Collinear Geometry at 28.6 MeV NUCLEAR REACTIONS 2H(p, 2p), E=28.6 MeV; measured σ. Collinear geometry, exact three-body calculation.
doi: 10.1103/PhysRevC.20.1585
1978SV01 Phys.Rev. C18, 983 (1978) Spin-Orbit Force and the Deformation of 12C NUCLEAR STRUCTURE 12C; calculated deformation.
doi: 10.1103/PhysRevC.18.983
1975BE48 Phys.Rev. C12, 2067 (1975) Interpretation of Inversions of Single-Particle Levels in Self-Consistent Field Theories NUCLEAR STRUCTURE 15N, 15,16O; calculated single-particle energies, level inversion.
doi: 10.1103/PhysRevC.12.2067
1974RE03 Phys.Rev. C9, 1882 (1974) N.E.Reid, N.E.Davison, J.P.Svenne Variational Calculation of Light Nuclei Using Nearly Orthogonal Functions NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated binding energies, radii, moments, density distributions. Variational method. Density-dependent interaction.
doi: 10.1103/PhysRevC.9.1882
1972PA21 Phys.Rev. C6, 34 (1972) How Good Is the Hartree-Fock Approximation for 16O (Question) NUCLEAR STRUCTURE 16O; analyzed intrinsic states; tested Hartree-Fock approximation.
doi: 10.1103/PhysRevC.6.34
1971CA24 Can.J.Phys. 49, 2028 (1971) Compressibility under Deformation of the Hartree-Fock Field NUCLEAR STRUCTURE 44Ca, 50Cr, 56,58Ni; calculated rms radius, compressibility under deformation. Deformed Hartree-Fock model.
doi: 10.1139/p71-245
1971LA05 Nucl.Phys. A164, 49 (1971) The Proton Densities in 40Ca and 48Ca in the Hartree-Fock Approximation NUCLEAR STRUCTURE 40,48Ca; calculated rms proton radii. Hartree-Fock theory.
doi: 10.1016/0375-9474(71)90842-6
1970BR37 Nucl.Phys. A154, 449 (1970) Isospin Mixing of Hartree-Fock Solutions NUCLEAR STRUCTURE 40,48Ca; calculated ground-state energy, proton, mass radii. Constrained Hartree-Fock method, isospin mixing.
doi: 10.1016/0375-9474(70)90117-X
1969CA08 Can.J.Phys. 47, 1393 (1969) Octupole Deformations in the 2s-1d Shell NUCLEAR STRUCTURE 30Si, 32,34S, 36,38Ar; calculated levels, deformation parameters.
doi: 10.1139/p69-178
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