NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = C.Wong Found 188 matches. Showing 1 to 100. [Next]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
2011WO04 Phys.Rev. C 84, 024901 (2011) Momentum-kick model description of the ridge in Δφ-Δη correlations in pp collisions at 7 TeV
doi: 10.1103/PhysRevC.84.024901
2010WO01 Phys.Rev. C 81, 064903 (2010) Anomalous soft photons in hadron production
doi: 10.1103/PhysRevC.81.064903
2009PI03 Phys.Rev. C 79, 024001 (2009) J.L.Ping, H.X.Huang, H.R.Pang, Fan Wang, C.W.Wong Quark models of dibaryon resonances in nucleon-nucleon scattering
doi: 10.1103/PhysRevC.79.024001
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
2004WO12 J.Phys.(London) G30, S1053 (2004) Does HBT measure the freeze-out source distribution?
doi: 10.1088/0954-3899/30/8/057
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
2000WO06 Phys.Rev. C61, 064011 (2000) Electroproduction of the d* Dibaryon NUCLEAR REACTIONS 2H(e, X), E=1 GeV; calculated two-Δ dibaryon production σ(θ). Several potentials compared.
doi: 10.1103/PhysRevC.61.064011
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
1999WO11 Phys.Rev. C60, 038201 (1999); Erratum Phys.Rev. C60, 069902 (1999) dππ Decay of the d* Dibaryon
doi: 10.1103/PhysRevC.60.038201
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
1998WO03 Phys.Rev. C57, 1962 (1998) Production and Decay of the d(*) Dibaryon NUCLEAR REACTIONS 2H(p, p'), E=516-2000 MeV; calculated d(*) dibaryon production σ(θ), decay width.
doi: 10.1103/PhysRevC.57.1962
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
1998WO13 Phys.Rev. C58, 2414 (1998) Three-Body Decay of the d* Dibaryon
doi: 10.1103/PhysRevC.58.2414
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
1994WO07 Int.J.Mod.Phys. E3, 821 (1994) Deuteron Radius and Nuclear Forces in Free Space NUCLEAR STRUCTURE 2H; compiled, reviewed data, analyses on radius.
doi: 10.1142/S0218301394000255
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
1992WO02 Nucl.Phys. A536, 269 (1992) The Deuteron Matter Radius NUCLEAR STRUCTURE 2H; calculated binding energy, matter radius. Realistic nucleon-nucleon potentials.
doi: 10.1016/0375-9474(92)90381-S
1992WO08 Nucl.Phys. A541, 384 (1992) Relativistic Channel-Coupling Effect in the Deuteron Matter Radius NUCLEAR STRUCTURE 2H; calculated matter radius, binding energy relativistic effect corrections. Dirac equations, local square-well, nonlocal separable potentials.
doi: 10.1016/0375-9474(92)90182-J
1992WO10 Phys.Lett. 291B, 363 (1992) Model Dependence in the Deuteron Matter Radius NUCLEAR STRUCTURE 2H; calculated matter radius; deduced quark, relativistic effects contributions.
doi: 10.1016/0370-2693(92)91387-O
1988WA08 Nucl.Phys. A480, 490 (1988) Quark Models of Nuclear Isobaric Energy Differences NUCLEAR STRUCTURE A=3-41; calculated isobaric energy differences. Quark model.
doi: 10.1016/0375-9474(88)90460-5
1988WA14 Nucl.Phys. A483, 661 (1988) Quark Models of 1S0 Nucleon-Nucleon Scattering Lengths NUCLEAR REACTIONS 1H(p, p), (n, n), 1n(n, n), E=low; calculated scattering length charge dependence quark contributions.
doi: 10.1016/0375-9474(88)90090-5
1986BR03 Phys.Rev. C33, 1235 (1986) V.R.Brown, C.Wong, C.H.Poppe, J.D.Anderson, J.C.Davis, S.M.Grimes, V.A.Madsen Cross Sections for the Ti(p, n) Reaction to Analogs of Ground and 2+ Excited States NUCLEAR REACTIONS, ICPND 46,47,48,49,50Ti(p, n), E=11.5-26 MeV; measured σ(En), σ(θ); deduced σ, β(n)/β(p). 46,48,50Ti levels deduced β.
doi: 10.1103/PhysRevC.33.1235
1986HA44 Phys.Rev. C34, 2075 (1986) L.F.Hansen, B.A.Pohl, C.Wong, R.C.Haight, Ch.Lagrange Measurements and Calculations of Neutron Scattering in the Actinide Region NUCLEAR REACTIONS 232Th, 238U, 239Pu(n, n), E=14.1 MeV; measured σ(E, θ=0°); deduced semi-microscopic, deformed optical model potentials.
doi: 10.1103/PhysRevC.34.2075
1986HE08 Phys.Lett. 168B, 177 (1986) Nucleon Core Size and Nuclear Forces NUCLEAR STRUCTURE 1n, 1H; calculated rms radius, nucleon quark core size.
doi: 10.1016/0370-2693(86)90959-7
1985BL12 Phys.Rev. C32, 411 (1985) M.Blann, S.M.Grimes, L.F.Hansen, T.T.Komoto, B.A.Pohl, W.Scobel, M.Trabandt, C.Wong Single-Particle Effects in Precompound Reactions: Influence of the f7/2 shell closure NUCLEAR REACTIONS 50,52,53Cr, 58Fe, 59Co, 60Ni, 63Cu(p, n), E=25 MeV; measured angle integrated neutron spectra; deduced precompound emission shell dependence.
doi: 10.1103/PhysRevC.32.411
1985FA01 Nucl.Phys. A432, 619 (1985) Coulomb Energies from Quark Exchanges between Nucleons NUCLEAR STRUCTURE 3H, 3He; A=5-15; calculated Coulomb energy differences. Resonating group method, quark exchange.
doi: 10.1016/0375-9474(85)90004-1
1985GR09 Phys.Rev. C31, 1679 (1985) S.M.Grimes, J.D.Anderson, J.C.Davis, R.H.Howell, C.Wong, A.W.Carpenter, J.A.Carr, F.Petrovich Gamow-Teller Matrix Elements from the 11B(p, n)11C Reaction at E(p) ≈ 26 MeV NUCLEAR REACTIONS, ICPND 11B(p, n), E=16-26 MeV; measured σ(En), σ(θ); deduced residual producation σ. 11C levels deduced Gamow-Teller matrix elements. DWA analysis, Cohen-Kurath wave functions, G-matrix based interactions.
doi: 10.1103/PhysRevC.31.1679
1985HA02 Phys.Rev. C31, 111 (1985) L.F.Hansen, F.S.Dietrich, B.A.Pohl, C.H.Poppe, C.Wong Test of Microscopic Optical Model Potentials for Neutron Elastic Scattering at 14.6 MeV over a Wide Mass Range NUCLEAR REACTIONS 9Be, C, 27Al, Fe, 59Co, 93Nb, 89Y, In, 140Ce, 181Ta, 197Au, 208Pb, 209Bi(n, n), E=14.6 MeV; measured σ(θ). Local microscopic potentials, optical model analysis.
doi: 10.1103/PhysRevC.31.111
1984LA21 Nucl.Phys. A423, 397 (1984) Relativistic Center-of-Mass Motion of Quarks in Bags NUCLEAR STRUCTURE 1H, 1n; calculated mass, μ. Bag model, relativistic center-of-mass motion.
doi: 10.1016/0375-9474(84)90031-9
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
1984SC33 Phys.Rev. C30, 1480 (1984) W.Scobel, M.Blann, T.T.Komoto, M.Trabandt, S.M.Grimes, L.F.Hansen, C.Wong, B.A.Pohl Single Particle Effects in Precompound Reactions NUCLEAR REACTIONS 50,52,53Cr, 54,56,58Fe, 59Co, 60Ni, 63Cu, 89Y, 90,91,92,94Zr, 92,94,96,97,98,100Mo, 110Pd, 159Tb(p, xn), E=25 MeV; 90,91,92,94Zr(p, xn), E=18 MeV; measured inclusive σ(En, θn); deduced precompound reaction single particle effects.
doi: 10.1103/PhysRevC.30.1480
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
1984WO06 Phys.Rev. C29, 1710 (1984) C.Wong, S.M.Grimes, R.W.Finlay Analysis of (p, p), (p, n), and (n, n) Scattering on the Even Tin Isotopes using the Lane Coupled Equations NUCLEAR REACTIONS 116,118,122,124Sn(p, n), E=24.5 MeV; measured σ(θ), σ(En); deduced isocalar, isovector strengths of potential. 116,120,124Sn(n, n), E=11 MeV; analyzed σ(θ); deduced potential parameters. Lane model, imaginary potential Coulomb correction.
doi: 10.1103/PhysRevC.29.1710
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
1983HA33 Phys.Rev. C28, 1934 (1983) L.F.Hansen, S.M.Grimes, C.H.Poppe, C.Wong Charge Exchange (p, n) Reactions to the Isobaric Analog States of High Z Nuclei: 73 ≤ Z ≤ 92 NUCLEAR REACTIONS 181Ta, 197Au, 209Bi, 232Th, 238U(p, n), E=27 MeV; measured σ(En), σ(θ). 232Th, 238U(p, p), (p, n), E=26 MeV; measured σ(θ). 181Ta, 197Au, 209Bi(n, n), E=8.05 MeV; 232Th(n, n), E=7 MeV; 238U(n, n), E=6.44, 7 MeV; analyzed σ(θ); deduced Lane potential validity. 181W, 197Hg, 209Po, 232Pa, 238Np deduced IAS excitation. Coupled-channels calculations.
doi: 10.1103/PhysRevC.28.1934
1983SC19 Z.Phys. A311, 323 (1983) W.Scobel, L.F.Hansen, B.A.Pohl, C.Wong, M.Blann Double Differential Cross Sections for (p, xn) Reactions of 64Zn, 65Cu and 89Y with 26 MeV Protons NUCLEAR REACTIONS 64Zn, 65Cu, 89Y(p, xn), E=26 MeV; measured inclusive σ(θn, En). Tof. Preequilibrium, hybrid model analysis.
doi: 10.1007/BF01415688
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
1982WO06 Phys.Rev. C26, 889 (1982) C.Wong, S.M.Grimes, C.H.Poppe, V.R.Brown, V.A.Madsen Excitation of 0+, 2+, (0+)', (2+)', 4+ Analog States in the Even Selenium Isotopes with 19-25 MeV Protons; Coupled-channel analysis NUCLEAR REACTIONS 76,80,82Se(p, n), E=19, 20, 22, 25 MeV; measured σ(En), σ(θ). 76,80,82Br deduced analog excitation mechanism. Coupled-channels calculation.
doi: 10.1103/PhysRevC.26.889
1981BR23 Phys.Rev. C24, 2359 (1981) V.R.Brown, C.Wong, S.M.Grimes, C.H.Poppe, V.A.Madsen Comment on ' Isospin and Strong-Coupling Effects in Neutron Scattering from Even-A Se Isotopes ' NUCLEAR REACTIONS 76,80,82Se(n, n), (n, n'), E=8 MeV; calculated σ(θ); deduced isospin optical model parameters. 76,80,82Se level deduced deformation parameters. Coupled-channels analysis.
doi: 10.1103/PhysRevC.24.2359
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
1980WO07 Phys.Rev. C22, 2523 (1980) Inelastic Production of Deuteron Bag States NUCLEAR REACTIONS 2H(e, e), (e, e'), E not given; calculated form factors; 2H(p, p'), (p, p'), E=0.89 GeV; calculated σ(θ); deduced circumstances for dinucleon color resonances.
doi: 10.1103/PhysRevC.22.2523
1979HA54 Nucl.Sci.Eng. 72, 35 (1979) L.F.Hansen, C.Wong, T.T.Komoto, B.A.Pohl, E.Goldberg, R.J.Howerton, W.M.Webster Neutron and Gamma-Ray Spectra from 232Th, 235U, 238U, and 239Pu after Bombardment with 14-MeV Neutrons NUCLEAR REACTIONS 232Th, 235,238U, 239Pu(n, n), (n, γ), E=14 MeV; measured σ(En, Eγ). Leakage spectra from pulsed spheres, tof, electron recoil technique.
doi: 10.13182/NSE79-A19307
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
1979WO05 Phys.Rev. C20, 59 (1979) C.Wong, V.R.Brown, V.A.Madsen, S.M.Grimes (p, n) Reaction to Ground- and Excited-State Analogs on the Samarium Isotopes: Importance of Two-Phonon Coupling Effects NUCLEAR REACTIONS 144,148,150,152Sm(p, n), E=20, 24.5, 26 MeV; measured σ(θ). 144,148,150,152Eu deduced analog states, deformation parameters. One-, two-phonon coupled channels calculations.
doi: 10.1103/PhysRevC.20.59
1978GR15 Phys.Rev. C18, 1100 (1978) S.M.Grimes, C.H.Poppe, C.Wong, B.J.Dalton Spin Cutoff Parameters for 28Si, 29Si, and 30P: Comparison of Measurements with Spectral Distribution Calculations NUCLEAR REACTIONS 25,26Mg, 27Al(α, n), E=10-18 MeV; measured σ(En, θ); deduced spin cutoff parameters for 28,29Si, 30P. Natural, enriched targets.
doi: 10.1103/PhysRevC.18.1100
1978WO14 Phys.Rev. C18, 2052 (1978) C.Wong, S.D.Bloom, S.M.Grimes, R.F.Hausman, Jr., V.A.Madsen Population of the 1+ Levels in 58Co via the 58Fe(p, n) Reaction NUCLEAR REACTIONS 58Fe(p, n), E=16, 19.1, 20.2 MeV; measured σ(θ). 58Co deduced 1+ strength distribution, fractional M1 strengths. Compared with reaction data, shell model calculations.
doi: 10.1103/PhysRevC.18.2052
1977FI10 Phys.Rev. C16, 2181 (1977) D.H.Fitzgerald, G.W.Greenlees, J.S.Lilley, C.H.Poppe, S.M.Grimes, C.Wong Energy Dependence of the 119Sn(p, n)119Sn (IAS) Reaction NUCLEAR REACTIONS 119Sn(p, n), E=16-20 MeV; measured σ(E, θ). 119Sb IAS deduced Γp/Γ, isospin form factor.
doi: 10.1103/PhysRevC.16.2181
1977HA25 Nucl.Sci.Eng. 62, 550 (1977) L.F.Hansen, T.Komoto, E.F.Plechaty, B.A.Pohl, G.S.Sidhu, C.Wong Measurements and Calculations of the Electron Recoil Spectra from Gamma Rays Emitted by Nitrogen for a 14-MeV Neutron Source NUCLEAR REACTIONS N(n, X), E=14 MeV; measured electron recoil spectra.
doi: 10.13182/NSE77-A26991
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