NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = W.Y.Hwang Found 23 matches. 2010BO05 Nucl.Phys. A832, 233 (2010) S.G.Bondarenko, V.V.Burov, W.-Y.P.Hwang, E.P.Rogochaya Relativistic multirank interaction kernels of the neutron-proton system
doi: 10.1016/j.nuclphysa.2009.11.002
2010BO23 Nucl.Phys. A848, 75 (2010) S.G.Bondarenko, V.V.Burov, W.-Y.P.Hwang, E.P.Rogochaya Covariant separable interaction for the neutron-proton system in 3S1-3D1 partial-wave state
doi: 10.1016/j.nuclphysa.2010.08.007
2008HW05 Phys.Rev. C 78, 025501 (2008) Parity-violating nuclear force as derived from QCD sum rules
doi: 10.1103/PhysRevC.78.025501
2005HW04 Eur.Phys.J. A 25, 467 (2005) Neutrons and antiprotons in ultrahigh-energy cosmic rays
doi: 10.1140/epja/i2005-10136-9
2003HW07 Nucl.Phys. A721, 1060c (2003) Electroweak Physics and Ultra High Energy Cosmic Rays
doi: 10.1016/S0375-9474(03)01285-5
2002HE12 Nucl.Phys. A706, 163 (2002) E.M.Henley, W.-Y.P.Hwang, L.S.Kisslinger Nonleptonic Hyperon Decays with QCD Sum Rules
doi: 10.1016/S0375-9474(02)00757-1
2001HW03 Nucl.Phys. A684, 167c (2001) Few-Nucleon Systems and QCD Sum Rules
doi: 10.1016/S0375-9474(01)00411-0
2000HW02 Nucl.Phys. A663-664, 1039c (2000) Green Functions in Large Nc QCD
doi: 10.1016/S0375-9474(99)00765-4
1999CH09 Phys.Lett. 451B, 283 (1999) Nucleon Spin Structure Functions in the Chiral Quark Model NUCLEAR STRUCTURE 1n, 1H; analyzed spin structure functions; deduced role of nonperturbative effects. Chiral quark model.
doi: 10.1016/S0370-2693(99)00226-9
1999HW03 Int.J.Mod.Phys. E8, 101 (1999) Muon Capture in Deuterium NUCLEAR REACTIONS 2H(μ-, nν), E at rest; calculated muon capture rates.
doi: 10.1142/S0218301399000070
1998HW01 Phys.Rev. C57, 61 (1998) W.-Y.P.Hwang, Z.-S.Yang, Y.S.Zhong, Z.N.Zhou, S.-L.Zhu QCD Sum Rules: Isospin symmetry breakings in pion-nucleon couplings
doi: 10.1103/PhysRevC.57.61
1998HW03 Nucl.Phys. A631, 487c (1998) Isospin Symmetry Breakings as from QCD Sum Rules
doi: 10.1016/S0375-9474(98)00053-0
1998ZH13 Phys.Lett. 420B, 8 (1998) Sh.-L.Zhu, W.-Y.P.Hwang, Z.-S.Yang Electromagnetic Decay of Vector Mesons as Derived from QCD Sum Rules
doi: 10.1016/S0370-2693(97)01524-4
1997HW04 Z.Phys. A358, 415 (1997) Semi-Inclusive Λ Production and Generalized Sullivan Processes
doi: 10.1007/s002180050349
1997WE10 Phys.Rev. C56, 3346 (1997) ρNN and ωNN Couplings in the External-Field QCD Sum Rule Method
doi: 10.1103/PhysRevC.56.3346
1996HE32 Phys.Lett. 367B, 21 (1996); Addendum Phys.Lett. 440B, 449 (1998) E.M.Henley, W.-Y.P.Hwang, L.S.Kisslinger The Weak Parity-Violating Pion-Nucleon Coupling NUCLEAR STRUCTURE 19F; analyzed parity violating limits, associated features. QCD sum rules.
doi: 10.1016/0370-2693(95)01403-9
1986CA23 Phys.Rev. C34, 1785 (1986) Importance of Quark Interchange in Pion Production via Nucleon-Nucleon Scattering NUCLEAR REACTIONS 2H(π+, π+), E=82, 142, 217 MeV; calculated σ(θ); 2H(π+, p), E not given; calculated absorption σ; 1H(n, pπ-), E not given; calculated σ(E(π), θ(π)); 1H(polarized p, π+), E=180 MeV; calculated analyzing power vs θ; 1H(n, pπ-), E not given; calculated analyzing power vs E. One gluon plus effective one-pion exchanges.
doi: 10.1103/PhysRevC.34.1785
1985HW01 Ann.Phys.(New York) 159, 118 (1985) Meson-Exchange Currents Including Energy Transfer Effects NUCLEAR REACTIONS 2H(γ, p), E=160-280 MeV; calculated photodisintegration σ(θ) vs E. Standard meson exchange current formalism, energy transfer effects.
doi: 10.1016/0003-4916(85)90194-0
1983HW01 Ann.Phys.(New York) 149, 335 (1983) W.-Y.P.Hwang, J.T.Londergan, G.E.Walker Deuteron Photodisintegration. I. Theory and Results at Low Energies NUCLEAR REACTIONS 2H(γ, p), E=20-140 MeV; calculated photodisintegration σ(θ). Elementary particle treatment.
doi: 10.1016/0003-4916(83)90201-4
1982HE09 Phys.Rev. C26, 2376 (1982) Effects of Nuclear Parity Violation in Deuterium Atoms and Elastic Electron-Deuteron Scattering NUCLEAR REACTIONS 2H(e, e'), E not given; calculated parity violating electromagnetic form factor, magnetization current vs convection current; deduced guage invariant constrained nucleon only impulse approximation validity.
doi: 10.1103/PhysRevC.26.2376
1982LI20 Ann.Phys.(New York) 143, 372 (1982) S.-P.Li, E.M.Henley, W.-Y.P.Hwang Parity Violation in Pion Electroproduction and Photoproduction with a Proton Target NUCLEAR REACTIONS 1H(γ, π0), (γ, π+), (polarized γ, π0), (polarized γ, π+), E=0.15-0.55 GeV; calculated production σ, asymmetry vs E. 1H(e, π0), (e, π+), (polarized e, π0), (polarized e, π+), E=800 MeV; calculated neutral weak current induced asymmetry. Parity violation effects.
doi: 10.1016/0003-4916(82)90032-X
1981HE06 Phys.Rev. C23, 1001 (1981); Erratum Phys.Rev. C24, 1374 (1981) Effects of Nuclear Parity Violation in Deuterium Atoms and Elastic Electron-Deuteron Scattering NUCLEAR REACTIONS 2H(e, e), E not given; calculated parity violating form factors. Gauge invariance constrained impulse approximation.
doi: 10.1103/PhysRevC.23.1001
1980HW01 Phys.Rev. C22, 968 (1980) Deuteron Photodisintegration: Impulse Approximation and Gauge Invariance NUCLEAR REACTIONS 2H(γ, p), E=10-120 MeV; calculated σ(θ). Impulse approximation vs gauge invariance.
doi: 10.1103/PhysRevC.22.968
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