NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = S.S.Wong Found 53 matches. 2000WO11 J.Phys.(London) G26, 1655 (2000) Inversion Technique for Hamiltonian Parameters in Finite-Shell Model Spaces
doi: 10.1088/0954-3899/26/11/302
1998SI17 Nucl.Data Sheets 84, 487 (1998) B.Singh, J.L.Rodriguez, S.S.M.Wong, J.K.Tuli Review of Log ft Values in β Decay COMPILATION A=1-250; compiled log ft values.
doi: 10.1006/ndsh.1998.0015
1997WO09 Nucl.Phys. A623, 431 (1997) A Finite Element Approach to the Two-Skyrmion Problem NUCLEAR STRUCTURE 2H; calculated binding energy. Finite element approach, Skyrme model, low-energy QCD.
doi: 10.1016/S0375-9474(97)00376-X
1994AZ03 Phys.Rev. C50, 1194 (1994); Erratum Phys.Rev. C56, 1655 (1997) R.E.Azuma, L.Buchmann, F.C.Barker, C.A.Barnes, J.M.D'Auria, M.Dombsky, U.Giesen, K.P.Jackson, J.D.King, R.G.Korteling, P.McNeely, J.Powell, G.Roy, J.Vincent, T.R.Wang, S.S.M.Wong, P.R.Wrean Constraints on the Low-Energy E1 Cross Section of 12C(α, γ)16O from the β-Delayed α Spectrum of 16N RADIOACTIVITY 16N(β-) [from on-line separation]; measured β-delayed α-spectrum, (α)(12C)-coin; deduced R-matrix, K-matrix level parameters relevant to 12C(α, γ) reaction. Thin Si surface barrier detector. NUCLEAR REACTIONS, ICPND 12C(α, γ), E(cm) ≤ 3 MeV; calculated E1 part of astrophysical S-factor, σ(E); deduced R-matrix, K-matrix level parameters. Data of β--delayed α-spectrum of 16N-decay input.
doi: 10.1103/PhysRevC.50.1194
1993BU03 Phys.Rev.Lett. 70, 726 (1993) L.Buchmann, R.E.Azuma, C.A.Barnes, J.M.D'Auria, M.Dombsky, U.Giesen, K.P.Jackson, J.D.King, R.G.Korteling, P.McNeely, J.Powell, G.Roy, J.Vincent, T.R.Wang, S.S.M.Wong, P.R.Wrean β-Delayed α Spectrum of 16N and the 12C(α, γ)16O Cross Section at Low Energies RADIOACTIVITY 16N(β-); measured β-delayed Eα, Iα, α(12C)-coin; deduced E1 part of 12C(α, γ) reaction, astrophysical S-factor.
doi: 10.1103/PhysRevLett.70.726
1993BU18 J.Phys.(London) G19, S115 (1993) L.Buchmann, R.E.Azuma, C.A.Barnes, A.Chen, J.Chen, J.M.D'Auria, M.Dombsky, U.Giesen, K.P.Jackson, J.D.King, R.Korteling, P.McNeely, J.Powell, G.Roy, M.Trinczek, J.Vincent, P.R.Wrean, S.S.M.Wong The β-Delayed α Spectrum of 16N and the Low-Energy Extrapolation of the 12C(α, γ)16O Cross Section RADIOACTIVITY 16N(β-); measured β-delayed Eα, Iα, βα-coin; deduced 12C(α, γ) reaction σ(E=low) implications.
doi: 10.1088/0954-3899/19/S/010
1993BU21 Nucl.Instrum.Methods Phys.Res. B79, 330 (1993) L.Buchmann, R.E.Azuma, C.A.Barnes, J.M.D'Auria, M.Dombsky, U.Giesen, K.P.Jackson, J.D.King, R.Korteling, P.McNeely, J.Powell, G.Roy, J.Vincent, S.S.M.Wong, P.R.Wrean A Study of Beta Delayed Alpha Emission from 16N RADIOACTIVITY 16N(β-); measured β-delayed α(12C)-coin. 18,17N(β-); measured β-delayed Eα, Iα; deduced 12C(α, γ) reaction p-wave capture amplitude.
doi: 10.1016/0168-583X(93)95357-B
1991KI08 Phys.Rev. C44, 1077 (1991) J.D.King, D.Frekers, R.Abegg, R.E.Azuma, L.Buchmann, C.Chan, T.E.Drake, R.Helmer, K.P.Jackson, L.Lee, C.A.Miller, E.Rost, R.Sawafta, R.Schubank, S.S.M.Wong, S.Yen, X.Q.Zhu Excitation of the 10.957 MeV 0-; T = 0 State in 16O by 400 MeV Protons NUCLEAR REACTIONS 16O(polarized p, p'), E=400 MeV; measured σ(θ), analyzing power vs θ; deduced reaction mechanism.
doi: 10.1103/PhysRevC.44.1077
1991NA11 Nucl.Phys. A530, 555 (1991) Neutron Structure Function and Deuteron EMC Effect NUCLEAR STRUCTURE 1n; analyzed data; deduced structure function, 2H EMC effect.
doi: 10.1016/0375-9474(91)90769-3
1989LE04 Nucl.Phys. A492, 607 (1989) L.Lee, T.E.Drake, S.S.M.Wong, D.Frekers, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Abegg, R.Helmer, K.P.Jackson, C.A.Miller, S.Yen Intermediate-Energy Proton Scattering to the Ground and Negative-Parity States of 40Ca, 90Zr and 208Pb NUCLEAR REACTIONS 40Ca(polarized p, p'), E=362 MeV; 90Zr(polarized p, p'), E=400 MeV; 208Pb(polarized p, p'), E=200, 400 MeV; measured σ(θ), A(y)(θ). Natural 40Ca, enriched 90Zr, 208Pb targets. Nonrelativistic microscopic density-dependent model analysis.
doi: 10.1016/0375-9474(89)90111-5
1989LE06 J.Phys.(London) G15, L91 (1989) L.Lee, T.E.Drake, S.S.M.Wong, D.Frekers, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Abegg, R.Helmer, K.P.Jackson, C.A.Miller, S.Yen Inelastic Proton Scattering to the Positive-Parity States in 90Zr at 400 MeV NUCLEAR REACTIONS 90Zr(polarized p, p'), E=400 MeV; measured σ(θ), A(θ). Enriched target. Nonrelativistic microscopic density-dependent model analysis.
doi: 10.1088/0954-3899/15/5/006
1988LE10 Phys.Lett. 205B, 219 (1988) L.Lee, T.E.Drake, S.S.M.Wong, D.Frekers, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Abegg, R.Helmer, K.P.Jackson, C.A.Miller, S.Yen, H.V.von Geramb Intermediate Energy Proton Scattering from 40Ca, 90Zr and 208Pb NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(polarized p, p), E=200, 362, 400 MeV; measured σ(θ), analyzing power vs θ, spin rotation parameter vs θ.
doi: 10.1016/0370-2693(88)91653-X
1988ZH01 Nucl.Phys. A476, 701 (1988) Static Properties of Chiral Soliton in a Nonlinear σ-Field with ρ-Meson Coupling NUCLEAR STRUCTURE 1n, 1H; calculated μ. Soliton model.
doi: 10.1016/0375-9474(88)90331-4
1987FR05 Phys.Rev. C35, 2236 (1987) D.Frekers, S.S.M.Wong, R.E.Azuma, T.E.Drake, J.D.King, R.Abegg, K.P.Jackson, C.A.Miller, S.Yen, W.P.Alford, R.L.Helmer, C.Broude, S.Mattsson, E.Rost Elastic and Inelastic Scattering of 362 MeV polarized Protons from 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=362 MeV; measured σ(θ), analyzing power. Magnetic spectrometer. Model calculations.
doi: 10.1103/PhysRevC.35.2236
1987MO13 Phys.Lett. 190B, 25 (1987) Symmetry in (p, p'γ) and Relativistic Models of Intermediate Energy Proton-Nucleus Scattering NUCLEAR REACTIONS 12C(p, p'γ), E=150, 500 MeV; calculated correlation function vs proton scattering angle. Relativistic models.
doi: 10.1016/0370-2693(87)90834-3
1987ZH08 Nucl.Phys. A466, 623 (1987) Impulse Approximation and Spin Observables in Inelastic Nucleon-Nucleus Scattering NUCLEAR REACTIONS 12C, 28Si(p, p'), (polarized p, p'), E=150, 200 MeV; calculated polarization, analyzing power, spin transfer parameters. Impulse approximation.
doi: 10.1016/0375-9474(87)90460-X
1986MI06 Phys.Lett. 169B, 166 (1986) C.A.Miller, A.Scott, R.Abegg, R.Helmer, K.P.Jackson, M.Whiten, S.Yen, L.Lee, T.E.Drake, D.Frekers, S.S.M.Wong, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Dymarz, H.V.von Geramb, C.J.Horowitz Large Angle Elastic Scattering of 200 MeV Protons from 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs θ; deduced exchange medium effects role. Microscopic Schrodinger, relativistic impulse approximation analyses.
doi: 10.1016/0370-2693(86)90643-X
1986MO12 Nucl.Phys. A456, 644 (1986) Gamma-Ray Angular Correlation in Intermediate Energy Proton-Nucleus Scattering NUCLEAR REACTIONS 12C(polarized p, p'γ), E=200 MeV; calculated γp(θ), γ-, proton polarization; deduced scattering amplitude independent parameters.
doi: 10.1016/0375-9474(86)90080-1
1986ZH04 Phys.Lett. 174B, 142 (1986) Difference between P and A(y) in forward Angle Inelastic Proton-Nucleus Scattering at Intermediate Energies NUCLEAR REACTIONS 12C(polarized p, p'), E=150 MeV; 24Mg, 28Si(polarized p, p'), E=200 MeV; calculated polarization, analyzing power difference vs θ; deduced kinematic effect role.
doi: 10.1016/0370-2693(86)90729-X
1985OX01 Z.Phys. A321, 485 (1985) K.Oxorn, S.K.Mark, J.E.Kitching, S.S.M.Wong High-Spin States in 89Nb, 88Zr and 88Nb with a Shell-Model Description of the N = 48 and N = 47 Nuclei NUCLEAR STRUCTURE 88,87Zr, 87Y, 88,89Nb, 90Mo; calculated levels. Shell model. NUCLEAR REACTIONS 89Y(α, 4n), (α, 4np), (α, 5n), E=54, 69 MeV; measured Eγ, Iγ, γγ-, γ(X-ray)-coin, γ(θ), neutron multiplicity. 88,89Nb, 88Zr deduced levels, J, π, γ-branching, γ-multipolarity.
doi: 10.1007/BF01411984
1985ZH01 Phys.Lett. 150B, 256 (1985) Scaling Law in the Electrodisintegration of Deuterons around 1(GeV/c)2 NUCLEAR REACTIONS 2H(e, e'), E not given; calculated photodisintegration σ(θ(e'), E(e')).
doi: 10.1016/0370-2693(85)91006-8
1985ZH07 Nucl.Phys. A439, 619 (1985) X.Zhu, R.E.Azuma, T.E.Drake, J.D.King, S.S.M.Wong Wolfenstein Parameters in the Helicity Representation for Intermediate-Energy Proton-Nucleus Scattering NUCLEAR REACTIONS 12C(polarized p, p), E=200 MeV; measured polarization, analyzing power, Wolfenstein parameters vs θ. Distorted wave approximation, momentum helicity representation.
doi: 10.1016/0375-9474(85)90330-6
1984WO12 Phys.Lett. 149B, 299 (1984) S.S.M.Wong, R.E.Azuma, T.E.Drake, J.D.King, X.Zhu Wolfenstein Parameters for 0+ → 0- Transitions Excited by Proton Scattering at Intermediate Energies NUCLEAR REACTIONS 16O(polarized p, p'), E=135 MeV; calculated σ(θ), analyzing power vs θ. 16O(polarized p, p'), E=200 MeV; calculated Wolfenstein parameters; deduced exchange term role. DWIA analysis.
doi: 10.1016/0370-2693(84)90410-6
1984YE01 J.Phys.(London) G10, L133 (1984) Oblate-Prolate Deformation in 28Si and Limitations of the Open-Shell Random-Phase Approximation NUCLEAR REACTIONS 28Si, 24Mg(e, e'), E not given; analyzed form factor data. 28Si deduced oblate, prolate transformations. Open shell RPA.
doi: 10.1088/0305-4616/10/6/005
1982HA45 Can.J.Phys. 60, 1502 (1982) Nuclear Level Densities NUCLEAR STRUCTURE 24,25Mg, 27Al, 28,29Si, 33S, 38Ar, 41Ca, 55Mn, 56Fe, 60Co, 60Ni; calculated level densities. Darwin-Fowler method, residual interaction folding.
doi: 10.1139/p82-202
1982WO07 Nucl.Phys. A389, 324 (1982) Binding Energy, Occupancy and Spin-Cutoff Factor Calculated by Statistical Spectroscopy with Configuration-Isospin Skewness and Excess Terms NUCLEAR STRUCTURE A=16-20; A=28; calculated binding energy, occupancy, spin cutoff factor. Shell model, isospin effects.
doi: 10.1016/0375-9474(82)90522-X
1981KA06 Phys.Lett. 98B, 393 (1981) A Shell Model Study of the Gamow-Teller Giant Resonance NUCLEAR STRUCTURE 21Mg; calculated β+-decay, Gamow-Teller strength function. SU(4) symmetry, statistical spectroscopy methods.
doi: 10.1016/0370-2693(81)90438-X
1980HA22 Phys.Lett. 93B, 357 (1980) Level Density in Large Spectroscopic Spaces NUCLEAR STRUCTURE 56Fe; calculated level densities, spin cutoff factor. Statistical, large spectroscopic space methods.
doi: 10.1016/0370-2693(80)90342-1
1978RO07 Nucl.Phys. A298, 31 (1978) D.J.Rowe, S.S.M.Wong, H.Chow, J.B.McGrory Isovector M6 Excitations in the Open-Shell Random Phase Approximation NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated isovector m6 excitations.
doi: 10.1016/0375-9474(78)90005-2
1978WO04 Nucl.Phys. A295, 275 (1978) Truncation of the Nuclear Shell-Model Space Using Spectral Strength Distribution NUCLEAR STRUCTURE 28Si; calculated levels.
doi: 10.1016/0375-9474(78)90116-1
1978WO05 Nucl.Phys. A295, 289 (1978) A Study of 28Si Using Shell-Model and Statistical Spectroscopic Methods NUCLEAR STRUCTURE 28Si; calculated levels, moment of inertia, B(λ).
doi: 10.1016/0375-9474(78)90117-3
1977VO06 Can.J.Phys. 55, 909 (1977) A Weak-Coupling Model for the Even Zn Isotopes NUCLEAR STRUCTURE 60,62,64,66,68Zn; calculated levels, B(E2), quadrupole moment.
doi: 10.1139/p77-122
1976LO08 Phys.Lett. 64B, 242 (1976) G.D.Lougheed, W.Y.Ng, S.S.M.Wong Truncation of the Shell Model Vector Space NUCLEAR STRUCTURE 24Mg; calculated levels, shell model truncation effect.
doi: 10.1016/0370-2693(76)90190-8
1976NG04 Can.J.Phys. 54, 2367 (1976) A Comparison of the Fixed-JT Averaging and Projected Hartree-Fock Methods for Nuclear Structure Studies NUCLEAR STRUCTURE 20,22,24,26Ne, 24,26,28Mg, 28,30,32Si, 32,34S, 36Ar; calculated levels.
doi: 10.1139/p76-284
1975LO05 Nucl.Phys. A246, 29 (1975) Constant Width Approximations for Large Spectroscopic Calculations NUCLEAR STRUCTURE 16O, 24Mg; calculated levels.
doi: 10.1016/0375-9474(75)90561-8
1974LO04 Nucl.Phys. A219, 171 (1974) N.Lo Iudice, D.J.Rowe, S.S.M.Wong 'Exact' Shell Model Calculations in A = 17 and A = 18 Nuclei and Effective Operators in the (2s, 1d) Shell NUCLEAR STRUCTURE A=17-18; calculated E2 effective charge, B(E2).
doi: 10.1016/0375-9474(74)90090-6
1974WO02 Phys.Lett. 48B, 403 (1974) S.S.M.Wong, D.J.Rowe, J.C.Parikh Calculations of the Giant Dipole Resonance for sd-Shell Nuclei in the Open-Shell Random Phase Approximation NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated giant dipole resonance.
doi: 10.1016/0370-2693(74)90364-5
1972PA03 Nucl.Phys. A182, 593 (1972) A Study of Some Measures for Group Symmetry Breaking in Nuclei
doi: 10.1016/0375-9474(72)90538-6
1972WO24 Nucl.Phys. A198, 188 (1972) Level-Density Fluctuations and Two-Body Versus Multi-Body Interactions
doi: 10.1016/0375-9474(72)90779-8
1971LO23 Phys.Lett. 37B, 44 (1971) N.Lo Iudice, D.J.Rowe, S.S.M.Wong A Shell-Model Calculation of the Mass 18 Nuclei and the Effective Interaction in the sh-Shell NUCLEAR STRUCTURE 18O, 18F; calculated levels. Shell model Kuo-Brown G-matrix elements.
doi: 10.1016/0370-2693(71)90565-X
1971RO03 Phys.Rev. C3, 73 (1971) D.J.Rowe, N.Ullah, S.S.M.Wong, J.C.Parikh, B.Castel Investigation of the One-Particle-Hole and Projected Hartree-Fock Approximations in C12 and O16 NUCLEAR STRUCTURE 12C, 16O; calculated levels, quadrupole moment. Particle-hole, projected Hartree-Fock approximations.
doi: 10.1103/PhysRevC.3.73
1970RO20 Nucl.Phys. A153, 561 (1970) The Open-Shell Random-Phase Approximation and the Negative Parity Excitations of 12C NUCLEAR STRUCTURE 12C; calculated negative-parity levels. Open-shell RPA.
doi: 10.1016/0375-9474(70)90792-X
1970UL01 Can.J.Phys. 48, 842 (1970) N.Ullah, S.S.M.Wong, L.E.H.Trainor Use of Perturbation Theory and Statistical Concepts in Nuclear Structure Studies with Application to the Ground State of 14N NUCLEAR STRUCTURE 14N; calculated ground-state properties. Perturbation, statistical theory.
doi: 10.1139/p70-107
1970WO15 Nucl.Phys. A159, 235 (1970) A Shell-Model Study of 65Cu and 63Cu NUCLEAR STRUCTURE 63,65Cu; calculated levels, quadrupole moment, B(λ). Shell model, realistic effective interaction.
doi: 10.1016/0375-9474(70)90039-4
1969RO26 Phys.Letters 30B, 147 (1969) Open-Shell RPA Calculations for the Giant-Dipole Excitations of 12C NUCLEAR STRUCTURE 12C; calculated giant dipole excitations. Open-shell random phase approximation.
doi: 10.1016/0370-2693(69)90351-7
1969UL03 Phys.Rev. 188, 1645 (1969) Mixed-Parity Hartree-Fock Calculations for Light Nuclei Using Realistic Forces NUCLEAR STRUCTURE 14,15N, 16,17,18O; calculated single-particle, binding energies. Hartree-Fock method, parity mixing.
doi: 10.1103/PhysRev.188.1645
1969WO05 Phys.Letters 30B, 150 (1969) The Giant Dipole Excitations of 12C in the Open Shell Tamm-Dancoff Approximation and in the Intermediate-Coupling Shell Model NUCLEAR STRUCTURE 12C; calculated giant dipole excitations. Tamm-Dancoff approximation, intermediate-coupling shell-model.
doi: 10.1016/0370-2693(69)90352-9
1968BU12 Nucl.Phys. A119, 184(1968) M.B.Burbank, G.G.Frank, N.E.Davison, G.C.Neilson, S.S.M.Wong, W.J.McDonald The 20Ne(d, n)21Na Reaction NUCLEAR REACTIONS 20Ne(d, n), E=3.92, 5.16, 6.08 MeV; measured σ(θ); 21Na levels deduced S. Enriched target.
doi: 10.1016/0375-9474(68)90813-0
1968WO03 Nucl.Phys. A113, 481 (1968) The (f7/2-1f7/2)2+ State in 48Sc NUCLEAR STRUCTURE 48Sc; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(68)90157-7
1968WO09 Phys.Letters 28B, 77 (1968) A Shell Model Study of the Structure of 56Ni NUCLEAR STRUCTURE 56Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90132-9
1966WO02 Phys.Letters 20, 188 (1966) Positive Parity States in 16O NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90930-9
1962WO02 Phys.Rev. 125, 280 (1962) Large-Angle Scattering of 18.7-MeV Alpha Particles by C12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.125.280
1960WO06 TID-13424 (1960) Large-Angle Scattering of 18.7-MeV Alpha Particles NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
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