NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = C.Y.Wong Found 84 matches. 2023WO02 Eur.Phys.J. A 59, 285 (2023) Dynamics of quarks and gauge fields in the lowest-energy states in QED and QCD interactions
doi: 10.1140/epja/s10050-023-01180-8
2022WO02 Eur.Phys.J. A 58, 100 (2022) On the stability of the open-string QED neutron and dark matter
doi: 10.1140/epja/s10050-022-00742-6
2021LE09 Phys.Lett. B 817, 136301 (2021) Pocket resonances in low-energy antineutron reactions with nuclei NUCLEAR REACTIONS C, Ag, Pb(n-bar, X), E=0.001-10 MeV; analyzed available data; deduced resonances using Bethe-Landau power law, antineutron-nucleus annihilation σ.
doi: 10.1016/j.physletb.2021.136301
2019CA04 Phys.Rev. C 99, 014606 (2019) X.G.Cao, E.J.Kim, K.Schmidt, K.Hagel, M.Barbui, J.Gauthier, S.Wuenschel, G.Giuliani, M.R.D.Rodriguez, S.Kowalski, H.Zheng, M.Huang, A.Bonasera, R.Wada, N.Blando, G.Q.Zhang, C.Y.Wong, A.Staszczak, Z.X.Ren, Y.K.Wang, S.Q.Zhang, J.Meng, J.B.Natowitz Examination of evidence for resonances at high excitation energy in the 7 α disassembly of 28Si NUCLEAR REACTIONS 12C(28Si, X), (28Si, 7α), E=35 MeV/nucleon; measured Eα, Iα, excitation functions for the α-conjugate exit channels using the 4π NIMROD-ISiS array for charged particle detection at the K500 superconducting cyclotron facility of Texas A and M. 28Si; deduced resonances at high excitation energies, shapes of 7α events in the de-excitation of projectile-like nuclei; calculated energies, J, π, configurations, quadrupole deformation of toroidal high-spin isomers using covariant functional PC-PK1 and DD-ME2.
doi: 10.1103/PhysRevC.99.014606
2018LE09 Phys.Rev. C 97, 054617 (2018) Optical model potential analysis of n(-bar)A and nA interactions NUCLEAR REACTIONS C, Al, Fe, Cu, Ag, Sn, Pb(n-bar, X), (n, X), (p-bar, X), E at 50-500 MeV/c; analyzed experimental data for annihilation reaction and nonelastic reaction channel σ(E) for antiparticle and neutron reactions by solving momentum-dependent optical model potential; deduced optical model potential well depth, power law dependence of annihilation σ on projectile momentum and atomic mass, and difference between antineutron-nucleus and antiproton-nucleus potentials.
doi: 10.1103/PhysRevC.97.054617
2018WO02 Phys.Rev. C 98, 034316 (2018) Shells in a toroidal nucleus in the intermediate-mass region
doi: 10.1103/PhysRevC.98.034316
2017ST08 Phys.Rev. C 95, 054315 (2017) A.Staszczak, C.-Y.Wong, A.Kosior Toroidal high-spin isomers in the nucleus 304120 NUCLEAR STRUCTURE 304120; calculated total Hartree-Fock-Bogoliubov (HFB) energy surface contour as a function of quadrupole and octupole moments, proton and neutron single-particle levels in the toroidal configuration as a function of quadrupole moment, particle-hole excitation configurations, proton and neutron single-particle Routhians, deformation energies as a function of quadrupole moment, toroidal high-spin isomers. Cranked self-consistent Skyrme-Hartree-Fock method.
doi: 10.1103/PhysRevC.95.054315
2017WO04 J.Phys.(London) G44, 075102 (2017) Event-by-event study of space-time dynamics in flux-tube fragmentation
doi: 10.1088/1361-6471/aa6fdb
2016LE03 Phys.Rev. C 93, 014616 (2016), Erratum Phys.Rev. C 95, 029901 (2017) Nuclear annihilation by antinucleons NUCLEAR REACTIONS 1,2H, 4He, Be, C, Ne, Al, Ni, Cu, Cd, Sn, Pt, Pb(p-bar, X), 1H, C, Al, Fe, Cu, Ag, Sn, Pb(n-bar, X), E at 20-1100 MeV/c; calculated antiproton-proton, antiproton-nucleus, antineutron-proton and antineutron-nucleus annihilation cross sections as functions of antiproton and antineutron momenta. Pomeranchuk's equality limit and extended Glauber model analysis. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.014616
2015SE02 Phys.Rev. C 91, 024901 (2015) A.Sen, J.Gerhard, G.Torrieri, K.Read, C.-Y.Wong Longitudinal hydrodynamics from event-by-event Landau initial conditions
doi: 10.1103/PhysRevC.91.024901
2015ST05 Acta Phys.Pol. B46, 675 (2015) Particle-hole Nature of the Light High-spin Toroidal Isomers NUCLEAR STRUCTURE 24Mg, 28Si, 32S, 36Ar, 40Ca, 44Ti, 48Cr, 52Fe; calculated excitation energies, quadrupole moments, density distributions of isomeric toroidal states. Comparison with available data.
doi: 10.5506/APhysPolB.46.675
2015ST17 Phys.Scr. 90, 114006 (2015) Toroidal high-spin isomers in light nuclei with N ≠ Z NUCLEAR STRUCTURE 28,32,34Si, 36,38S, 40,42Ar, 40Ca, 44Ti, 48Cr, 52Fe; calculated single-particle states, total HFB and isomeric toroidal states energies, quadrupole moments. Comparison with available data.
doi: 10.1088/0031-8949/90/11/114006
2014LE11 Phys.Rev. C 89, 054601 (2014) Extended Glauber model of antiproton-nucleus annihilation for all energies and mass numbers NUCLEAR REACTIONS 1,2H, 4He, Be, C, Ne, Al, Ni, Cu, Cd, Sn, Pt, Pb(p-bar, X), E at 10-3000 MeV/c; calculated antiproton-nucleus annihilation σ(E) based on extended Glauber model. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.054601
2014WO04 Phys.Rev. C 90, 064907 (2014) C.-Y.Wong, A.Sen, J.Gerhard, G.Torrieri, K.Read Analytical solutions of Landau (1+1)-dimensional hydrodynamics
doi: 10.1103/PhysRevC.90.064907
2012WO04 Phys.Rev. C 85, 064909 (2012) Bose-Einstein interference in the passage of a jet in a dense medium
doi: 10.1103/PhysRevC.85.064909
2012WO08 Phys.Rev. C 86, 064603 (2012) Reaction cross sections in heavy-ion collisions NUCLEAR REACTIONS 16O(14N, X), E=3-18 MeV; 16O(16O, X), E=5-35 MeV; 12C(13C, X), E=2-8 MeV; 12C(12C, X), E=2.8-6.5 MeV; calculated fusion σ, barrier heights, penetration probability. Continuum approximation for all partial waves. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.064603
2012WO09 J.Phys.:Conf.Ser. 387, 012009 (2012) Novel Bose-Einstein Interference in the Passage of a Fast Particle in a Dense Medium
doi: 10.1088/1742-6596/387/1/012009
2010WO01 Phys.Rev. C 81, 064903 (2010) Anomalous soft photons in hadron production
doi: 10.1103/PhysRevC.81.064903
2009ST09 Acta Phys.Pol. B40, 753 (2009) Toroidal Super-Heavy Nuclei in Skyrme-Hartree-Fock Approach
2009WO03 Phys.Rev. C 80, 034908 (2009) Momentum kick model analysis of PHENIX near-side ridge data and photon jet
doi: 10.1103/PhysRevC.80.034908
2009WO04 Phys.Rev. C 80, 054917 (2009) Wigner function of produced particles in string fragmentation
doi: 10.1103/PhysRevC.80.054917
2008WO05 Phys.Rev. C 78, 054902 (2008) Landau hydrodynamics reexamined
doi: 10.1103/PhysRevC.78.054902
2008WO06 Phys.Rev. C 78, 064905 (2008) Momentum kick model description of the near-side ridge and jet quenching
doi: 10.1103/PhysRevC.78.064905
2008YU02 Phys.Rev. C 78, 014908 (2008) L.-Li.Yu, W.-N.Zhang, C.-Y.Wong Hanbury-Brown - Twiss interferometry with quantum transport of the interfering pair
doi: 10.1103/PhysRevC.78.014908
2007PA41 Phys.Rev. C 76, 044907 (2007) Y.Park, K.-I.Kim, T.Song, S.H.Lee, C.-Y.Wong Widths of quarkonia in quark gluon plasma
doi: 10.1103/PhysRevC.76.044907
2007WO03 Phys.Rev. C 76, 014902 (2007) Quarkonia and quark drip lines in a quark-gluon plasma
doi: 10.1103/PhysRevC.76.014902
2007WO05 Phys.Rev. C 76, 034905 (2007) Chaoticity parameter λ in Hanbury-Brown - Twiss interferometry
doi: 10.1103/PhysRevC.76.034905
2007WO09 Phys.Rev. C 76, 054908 (2007) Ridge structure in the Δφ - Δη correlation function associated with a near-side jet
doi: 10.1103/PhysRevC.76.054908
2006WO11 J.Phys.(London) G32, S301 (2006) Heavy quarkonia and quark drip lines in quark-gluon plasma
doi: 10.1088/0954-3899/32/12/S37
2006ZH25 Phys.Rev. C 74, 024908 (2006) W.-N.Zhang, Y.-Y.Ren, C.-Y.Wong Analysis of pion elliptic flow and Hanbury-Brown-Twiss interferometry in a granular quark-gluon plasma droplet model NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed pions transverse momentum, elliptic flow, correlations; deduced expanding source of granular droplets.
doi: 10.1103/PhysRevC.74.024908
2005WO08 Phys.Rev. C 72, 034906 (2005) Heavy quarkonia in quark-gluon plasma
doi: 10.1103/PhysRevC.72.034906
2005ZH21 Phys.Rev. C 71, 064908 (2005) W.-N.Zhang, S.-X.Li, Ch.-Y.Wong, M.J.Efaaf Signals in single-event pion interferometry for granular sources of quark-gluon plasma droplets
doi: 10.1103/PhysRevC.71.064908
2004WO08 Phys.Rev. C 69, 055202 (2004) Molecular states of heavy quark mesons
doi: 10.1103/PhysRevC.69.055202
2004WO18 Phys.Rev. C 70, 064904 (2004) Signature of granular structures by single-event intensity interferometry
doi: 10.1103/PhysRevC.70.064904
2004ZH29 Phys.Rev. C 70, 024903 (2004) W.N.Zhang, M.J.Efaaf, C.-Y.Wong Pion interferometry for a granular source of quark-gluon plasma droplets
doi: 10.1103/PhysRevC.70.024903
2004ZH32 Chin.Phys.Lett. 21, 1918 (2004) W.-N.Zhang, M.J.Efaaf, C.-Y.Wong, M.Khaliliasr Pion Interferometry for Hydrodynamical Expanding Source with a Finite Baryon Density
doi: 10.1088/0256-307X/21/10/015
2003WO02 Nucl.Phys. A715, 541c (2003) C.-Y.Wong, T.Barnes, E.S.Swanson, H.W.Crater The Role of Produced Hadrons in J/ψ Suppression
doi: 10.1016/S0375-9474(02)01511-7
2003WO05 J.Phys.(London) G29, 2151 (2003) Intensity interferometry for a chaotic source with a collective flow and multiple scattering
doi: 10.1088/0954-3899/29/9/310
2003XU03 Phys.Rev. C 67, 014907 (2003) Anomalous J/ψ suppression and charmonium dissociation cross sections NUCLEAR REACTIONS Pb(Pb, X), E=high; analyzed J/ψ production σ, dependence on temperature-dependent charmonium dissociation cross section.
doi: 10.1103/PhysRevC.67.014907
2003ZH27 Phys.Rev. C 68, 035211 (2003) Total hadron-hadron cross sections at high energies NUCLEAR REACTIONS 1H(p, X), (π+, X), (π-, X), (K+, X), (K-, X), E(cm) ≈ 10-300 GeV; calculated total σ. Other hadron-hadron cross sections also calculated. Low-Nussinov two-gluon model.
doi: 10.1103/PhysRevC.68.035211
2002WO01 Phys.Rev. C65, 014903 (2002); Erratum Phys.Rev. C66, 029901 (2002) C.-Y.Wong, E.S.Swanson, T.Barnes Heavy Quarkonium Dissociation Cross Sections in Relativistic Heavy-Ion Collisions
doi: 10.1103/PhysRevC.65.014903
2002WO06 Phys.Rev. C65, 034902 (2002) Dissociation of a Heavy Quarkonium at High Temperatures
doi: 10.1103/PhysRevC.65.034902
2002WO09 J.Phys.(London) G28, 2349 (2002) Dissociation of Heavy Quarkonia in the Quark-Gluon Plasma
doi: 10.1088/0954-3899/28/9/302
2001WO02 Nucl.Phys. A681, 22c (2001) Signatures of Quark-Gluon Plasma Phase Transition in High-Energy Nuclear Collisions
doi: 10.1016/S0375-9474(00)00477-2
2001WO05 Phys.Rev. C63, 044907 (2001) Relativtic N-Body Problem in a Separable Two-Body Basis
doi: 10.1103/PhysRevC.63.044907
2000WO09 Phys.Rev. C62, 045201 (2000) C.-Y.Wong, E.S.Swanson, T.Barnes Cross Sections for π- and ρ-Induced Dissociation of J/ψ and ψ'
doi: 10.1103/PhysRevC.62.045201
2000YO03 Phys.Rev. C61, 044905 (2000) Relativistic Modification of the Gamow Factor
doi: 10.1103/PhysRevC.61.044905
1998WO02 Nucl.Phys. A630, 487c (1998) Signatures of Absorption Mechanisms for J/ψ and ψ' Production in High-Energy Heavy-Ion Collisions
doi: 10.1016/S0375-9474(97)00788-4
1998WO05 Phys.Rev. C58, 376 (1998) Effects of Parton Intrinsic Transverse Momentum on Photon Production in Hard-Scattering Processes
doi: 10.1103/PhysRevC.58.376
1997WO03 Phys.Rev. C55, 2621 (1997) Suppression of J/ψ and ψ' Production in High-Energy Pb on Pb Collisions NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; analyzed data; deduced anomalous J/ψ suppression is dependent on phase transition due to local energy density exceeding a certain value.
doi: 10.1103/PhysRevC.55.2621
1996WO03 Phys.Rev.Lett. 76, 196 (1996) Suppression of ψ' and J/ψ in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS U(S, X), (O, X), Cu(O, X), (p, X), 1H(p, X), E=high; analyzed ψ' to J/ψ ratio; deduced c(c-bar)-baryon absorption σ related features.
doi: 10.1103/PhysRevLett.76.196
1996WO14 Nucl.Phys. A610, 434c (1996) J/ψ and ψ' Suppression in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), E at 158 GeV/c/nucleon; analyzed J/ψ production suppression data; deduced local energy density role.
doi: 10.1016/S0375-9474(96)00375-2
1996WO16 Phys.Lett. 367B, 50 (1996) Excess Dileptons in High-Energy Nucleus-Nucleus Collisions NUCLEAR REACTIONS U(S, X), E=200 GeV/nucleon; calculated μ+μ--yield; deduced dilepton enhanced yield related features. Open charm production approach.
doi: 10.1016/0370-2693(95)01471-3
1995CH14 Phys.Rev. C51, 2125 (1995) Correction Factors for Reactions Involving q(q-bar) Annihilation or Production
doi: 10.1103/PhysRevC.51.2125
1995MO03 Phys.Rev. C51, 2135 (1995) Boundary and Coulomb Effects on Boson Systems in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS S(S, X), E=200 GeV/nucleon; 197Au(O, X), E=200 GeV/nucleon; analyzed data; deduced boson systems' boundary, Coulomb effects role.
doi: 10.1103/PhysRevC.51.2135
1994XU02 Nucl.Phys. A569, 575 (1994) H.M.Xu, C.A.Gagliardi, R.E.Tribble, C.Y.Wong Multifragmentation of Toroidal and Bubble Nuclei within the BUU Approach NUCLEAR REACTIONS 92Mo(92Mo, X), E=75, 85, 100 MeV/nucleon; calculated compressed state, average density, transverse excitation energy time evolution; deduced multi-fragmentation evidence. Improved Boltzmann-Uehling-Uhlenbeck model.
doi: 10.1016/0375-9474(94)90320-4
1994XU04 Phys.Rev. C49, R1778 (1994) H.M.Xu, C.A.Gagliardi, R.E.Tribble, C.Y.Wong Fragmentation Barriers of Toroidal and Bubble Nuclei NUCLEAR REACTIONS 92Mo(92Mo, X), E=75 MeV/nucleon; calculated toroidal, bubble nuclei formation deformation energy surfaces; deduced fragmentation barrier time evolution. Improved Boltzmann-Uehling-Uhlenbeck model.
doi: 10.1103/PhysRevC.49.R1778
1993XU03 Phys.Rev. C48, 933 (1993) H.M.Xu, J.B.Natowitz, C.A.Gagliardi, R.E.Tribble, C.Y.Wong, W.G.Lynch Formation and Decay of Toroidal and Bubble Nuclei and the Nuclear Equation of State NUCLEAR REACTIONS 92Mo(92Mo, X), E=75-100 MeV/nucleon; calculated multi-fragment decay multiplicity. Stiff, soft equations of state, toroidal, bubble nuclei formation.
doi: 10.1103/PhysRevC.48.933
1984MA17 Z.Phys. A316, 35 (1984) A.D.MacKellar, G.R.Satchler, C.-Y.Wong An Exploratory Study of Antiproton-Nucleus Scattering NUCLEAR REACTIONS 16O(p-bar, p-bar), E=45, 175 MeV; calculated σ(θ).12C(p-bar, p-bar), E=50-200 MeV; calculated reaction σ(E).208Pb(p-bar, p-bar), E=70 MeV; calculated reaction σ vs real, imaginary potential parameters. Antiproton-atom data derived potentials.
doi: 10.1007/BF01415658
1984WO01 Phys.Rev. C29, 574 (1984) C.-Y.Wong, A.K.Kerman, G.R.Satchler, A.D.MacKellar Ambiguity in Antiproton-Nucleus Potentials from Antiprotonic-Atom Data NUCLEAR REACTIONS 12C(p-bar, p-bar), E=70 MeV; calculated σ(θ); deduced potential ambiguities. Optical potentials from p-bar atomic data.
doi: 10.1103/PhysRevC.29.574
1984WO11 Phys.Rev. C30, 1949 (1984) Rotating Toroidal Nuclei in Heavy-Ion Reactions NUCLEAR REACTIONS 58Ni(35Cl, X), (32S, X), E ≈ 11 MeV/nucleon; calculated three fragment breakup probability; deduced intermediate 93,95Rh toroidal nucleus role.
doi: 10.1103/PhysRevC.30.1949
1983AU06 Phys.Rev. C28, 1552 (1983) R.L.Auble, J.B.Ball, F.E.Bertrand, C.B.Fulmer, D.C.Hensley, I.Y.Lee, R.L.Robinson, P.H.Stelson, C.Y.Wong, D.L.Hendrie, H.D.Holmgren, J.D.Silk Light Ion Emission from Reactions Induced by 0.8-2.4 GeV 16O Projectiles NUCLEAR REACTIONS Ni(16O, X), E=0.8, 1.6, 2.4 GeV; Au(16O, X), E=1.6, 2.4 GeV; Al, Sn(16O, X), E=1.6 GeV; measured σ(E, θ) for X=p, d, t, 3He, 4He; deduced model parameters.
doi: 10.1103/PhysRevC.28.1552
1983WO08 Phys.Rev. C28, 240 (1983) Approximate Treatment of Particle Collisions in the Time-Dependent Mean-Field Theory NUCLEAR REACTIONS 40Ca(16O, X), 28Si(28Si, X), E=100 MeV/nucleon; calculated density contours. TDHF, particle collisions.
doi: 10.1103/PhysRevC.28.240
1980TA09 Phys.Rev. C21, 1846 (1980) Exactly Central Heavy-Ion Collisions by Nuclear Hydrodynamics NUCLEAR REACTIONS 197Au(20Ne, X), 208Pb(208Pb, X), E=50, 100, 250, 400 MeV/nucleon; calculated σ(fragment θ, E); deduced nuclear viscosity, thermal conductivity effects. Hydrodynamical model.
doi: 10.1103/PhysRevC.21.1846
1980WO06 Phys.Lett. B96, 258 (1980) Influence of Particle Collisions on the Time-dependent Hartree-Fock Fusion Window in 16O + 40Ca NUCLEAR REACTIONS 40Ca(16O, X), E=168 MeV; calculated neutron occupation probability vs time; deduced fusion window threshold, influence of particle collisions. Extended TDHF method.
doi: 10.1016/0370-2693(80)90761-3
1979VA12 Phys.Rev.Lett. 43, 840 (1979) K.Van Bibber, D.L.Hendrie, D.K.Scott, H.H.Wieman, L.S.Schroeder, J.V.Geaga, S.A.Cessin, R.Treuhaft, Y.J.Grossiord, J.O.Rasmussen, C.Y.Wong Evidence for Orbital Dispersion in the Fragmentation of 16O at 90 and 120 MeV/Nucleon NUCLEAR REACTIONS Al, Au(16O, 7Be), (16O, 11B), (16O, 14N), E=90, 120 MeV/nucleon; measured σ(θ); deduced evidence for orbital deflection of projectile before breakup. Discussed statistical model vs abrasion-ablation model.
doi: 10.1103/PhysRevLett.43.840
1976SH06 Phys.Lett. 61B, 29 (1976) R.E.Shamu, C.H.Lagrange, E.M.Bernstein, J.J.Ramirez, T.Tamura, C.Y.Wong Quadrupole Deformation Parameters of 148,152,154Sm Determined from Neutron Total Cross Sections NUCLEAR REACTIONS 148,152,154Sm(n, X), E=0.75-14.5 MeV; measured relative σ. 148,152,154Sm deduced β.
doi: 10.1016/0370-2693(76)90553-0
1976WO07 Phys.Rev.Lett. 37, 664 (1976); Erratum Phys.Rev.Lett. 37, 1367 (1976) Primordial Superheavy Element 126
doi: 10.1103/PhysRevLett.37.664
1975KO08 Nucl.Phys. A245, 205 (1975) Shape Isomerism in Mercury Isotopes NUCLEAR STRUCTURE 184,186,188,200Hg; calculated levels.
doi: 10.1016/0375-9474(75)90173-6
1973DA35 Nucl.Phys. A216, 250 (1973) K.T.R.Davies, S.J.Krieger, C.Y.Wong Generalized Shells in Nuclei; Hartree-Fock Calculations for Bubble Nuclei NUCLEAR STRUCTURE 36Ar, 68,84Se, 100Sn, 116,138Ce, 200Hg; calculated level densities.
doi: 10.1016/0375-9474(73)90467-3
1973WO07 Phys.Rev.Lett. 31, 766 (1973) Interaction Barrier in Charged-Particle Nuclear Reactions NUCLEAR REACTIONS, Fission 238U(α, F), (11B, F), (14N, F), (16O, F), (40Ar, F); calculated σ(E).
doi: 10.1103/PhysRevLett.31.766
1972BR23 Rev.Mod.Phys. 44, 320 (1972) M.Brack, J.Damgaard, A.S.Jensen, H.C.Pauli, V.M.Strutinsky, C.Y.Wong Funny Hills: the Shell-Correction Approach to Nuclear Shell Effects and its Applications to the Fission Process
doi: 10.1103/RevModPhys.44.320
1972DA30 Phys.Lett. 41B, 455 (1972) K.T.R.Davies, C.Y.Wong, S.J.Krieger Hartree-Fock Calculations of Bubble Nuclei NUCLEAR STRUCTURE 36Ar, 200Hg; calculated mass, nucleon densities. Hartree-Fock theory.
doi: 10.1016/0370-2693(72)90673-9
1972KR03 Phys.Rev.Lett. 28, 690 (1972) Validity of Strutinsky's Theory of Renormalization NUCLEAR STRUCTURE 32S; calculated total energy, nuclear deformation energy surface. Strutinsky theory.
doi: 10.1103/PhysRevLett.28.690
1972WO25 Part.Nucl. 4, 163 (1972) C.Y.Wong, T.Tamura, H.Marshak, A.Langsford Effects of Nuclear Collectivity on the Total Neutron Cross Section NUCLEAR REACTIONS 165Ho, 112Cd, 164Dy(n, X), E < 30 MeV; analyzed σ(nT)(E); deduced nuclear collectivity effects.
1972WO27 Phys.Lett. 42B, 186 (1972) Fusion Threshold Energy in Heavy-Ion Reactions
doi: 10.1016/0370-2693(72)90056-1
1972WO28 Phys.Lett. 41B, 446 (1972) Toroidal Nuclei
doi: 10.1016/0370-2693(72)90671-5
1972WO29 Phys.Lett. 41B, 451 (1972) Bubble Nuclei NUCLEAR STRUCTURE 36Ar, 84Se, 138Ce, 174Yb, 200Hg, 250Rf; calculated shell-corrected deformation energies, single-particle energies. Strutinsky renormalization theory.
doi: 10.1016/0370-2693(72)90672-7
1970FO01 Nucl.Phys. A142, 525 (1970) J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, T.Tamura, C.-Y.Wong Elastic and Inelastic Proton Scattering from 109Ag NUCLEAR REACTIONS 109Ag(p, p'), E=13 MeV; measured σ(θ). 109Ag deduced levels, deformation parameters. Enriched target.
doi: 10.1016/0375-9474(70)90810-9
1970MA43 Phys.Rev. C2, 1862 (1970) H.Marshak, A.Langsford, T.Tamura, C.Y.Wong Total Neutron Cross Section of Oriented 165Ho from 2 to 135 MeV NUCLEAR REACTIONS 165Ho(n, X), E=2-135 MeV; measured σ(nT)(E). Oriented target.
doi: 10.1103/PhysRevC.2.1862
1970WO12 Phys.Lett. 32B, 668 (1970) Shells in a Simple Anisotropic Harmonic Oscillator NUCLEAR STRUCTURE 8Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated single-particle states vs deformation. Anisotropic harmonic oscillator model.
doi: 10.1016/0370-2693(70)90439-9
1969RO30 Phys.Rev. 187, 1609 (1969) R.L.Robinson, J.L.C.Ford, Jr., P.H.Stelson, T.Tamura, C.Y.Wong Elastic and Inelastic Proton Scattering from 110Pd NUCLEAR REACTIONS 110Pd(p, p), (p, p'), E=13 MeV; measured σ(Ep', θ). 110Pd deduced levels, J, π, β(L).
doi: 10.1103/PhysRev.187.1609
1968ST18 Nucl.Phys. A119, 14 (1968) P.H.Stelson, J.L.C.Ford, Jr., R.L.Robinson, C.Y.Wong, T.Tamura Elastic and Inelastic Proton Scattering from 112,114Cd NUCLEAR REACTIONS 112,114Cd(p, p), (p, p'), E=13 MeV; measured σ(Ep, θ), σ(Ep', θ). 112,114Cd deduced levels, deformation parameters β(L). Enriched targets. DWBA, coupled-channel calculations.
doi: 10.1016/0375-9474(68)90802-6
1967FO08 Phys.Rev. 158, 1194 (1967) J.L.C.Ford, Jr., C.-Y.Wong, T.Tamura, R.L.Robinson, P.H.Stelson Elastic and Inelastic Proton Scattering from 107Ag and the Phonon-Core Model NUCLEAR STRUCTURE 107Ag; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.158.1194
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