NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.Y.Cheung Found 12 matches. 2005MI21 Nucl.Phys. A755, 571c (2005) Generalized parton distributions of the nucleon based on the Faddeev approach to the NJL model
doi: 10.1016/j.nuclphysa.2005.03.071
2005MI24 Phys.Rev. C 72, 025202 (2005) H.Mineo, S.N.Yang, C.-Y.Cheung, W.Bentz Generalized parton distributions of the nucleon in the Nambu-Jona-Lasinio model based on the Faddeev approach NUCLEAR STRUCTURE 1H; calculated spin-averaged and helicity-flip generalized parton distributions. Nambu-Jona-Lasinio model.
doi: 10.1103/PhysRevC.72.025202
2000CH12 Nucl.Phys. A663-664, 667c (2000) Nonperturbative Determination of Heavy Meson Bound States
doi: 10.1016/S0375-9474(99)00710-1
1991CH08 Nucl.Phys. A526, 674 (1991) Compton Scattering by the Proton and Nucleon Polarizabilities NUCLEAR REACTIONS 1H(γ, γ), E=low; calculated Compton scattering σ(θ), asymmetry; deduced nucleon polarizabilities role.
doi: 10.1016/0375-9474(91)90437-B
1988MC03 Phys.Rev.Lett. 61, 814 (1988) J.P.McDermott, E.Rost, J.R.Shepard, C.Y.Cheung Relativistic (γ, p) Calculations at Intermediate Energies NUCLEAR REACTIONS 16O(γ, p), E=196 MeV; 40Ca(γ, p), E=100-300 MeV; calculated σ(θ).
doi: 10.1103/PhysRevLett.61.814
1988SH07 Phys.Rev. C37, 1130 (1988) J.R.Shepard, E.Rost, C.-Y.Cheung, J.A.McNeil Magnetic Response of Closed-Shell ±1 Nuclei in Dirac-Hartree Approximation NUCLEAR REACTIONS 15N(e, e), E not given; calculated isoscalar M1 form factor. Dirac-Hartree approximation. NUCLEAR STRUCTURE 15N, 15O; A=15, 17, 39, 41; calculated μ. Dirac-Hartree approximation.
doi: 10.1103/PhysRevC.37.1130
1986CH05 Phys.Rev. C33, 776 (1986) Role of the Δ(1232) in the (γ, p) Reaction NUCLEAR REACTIONS 16O, 4He(γ, p), E=100-300 MeV; calculated σ(θ); deduced isobar role.
doi: 10.1103/PhysRevC.33.776
1986MA21 Nucl.Phys. A454, 606 (1986) Two-Body Absorption of Pions in 3He NUCLEAR REACTIONS 3He(π+, 2p), (π-, np), E ≈ 20-180 MeV; calculated σ(E), σ(θ). 3He deduced σ(π+)/σ(π-). Two-body pion absorption, rescattering effects.
doi: 10.1016/0375-9474(86)90108-9
1984CH32 Phys.Lett. 149B, 18 (1984) Pion Effect in Deep-Inelastic Polarized-Lepton-Polarized-Nucleon Scattering NUCLEAR REACTIONS 1H(polarized e, e'), E not given; calculated asymmetry; deduced nucleon quark spin polarization.
doi: 10.1016/0370-2693(84)91542-9
1983CH25 Phys.Lett. 127B, 147 (1983) Electro-Disintegration of 2H with Polarized Beam and Target NUCLEAR REACTIONS 2H(polarized e, e'n), (polarized e, e'X), E=1 GeV; calculated electrodisintegration σ(θ(e), θp) vs outgoing electron momentum, asymmetry vs θ; deduced neutron electric form factor dependence. Quasifree, fixed kinematics, longitudinal beam polarization, polarized target.
doi: 10.1016/0370-2693(83)90863-8
1982CH27 Phys.Lett. 119B, 47 (1982) Charge Symmetry and the Reaction d + d → 4He + π0 NUCLEAR REACTIONS 2H(d, π0), E=500-700 MeV; calculated σ(θ=0°). T-matrix approach, different charge symmetry breaking mechanisms.
doi: 10.1016/0370-2693(82)90240-4
1980CH27 Nucl.Phys. A348, 365 (1980) C.Y.Cheung, E.M.Henley, G.A.Miller Charge Symmetry Breaking in the Neutron-Proton System NUCLEAR REACTIONS 1H(n, n), E=160, 300 MeV; calculated polarization difference vs θ. 1H(n, d), E=577 MeV; calculated σ(θ). Charge symmetry breaking mechanism.
doi: 10.1016/0375-9474(80)90261-4
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