NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.W.Chen Found 30 matches. 2020LY02 J.Phys.(London) G47, 045109 (2020) J.E.Lynn, D.Lonardoni, J.Carlson, J.-W.Chen, W.Detmold, S.Gandolfi, A.Schwenk Ab initio short-range-correlation scaling factors from light to medium-mass nuclei NUCLEAR STRUCTURE 2,3H, 3,4,6He, 6Li, 12C, 16O, 40Ca, 63Cu, 56Fe, 197Au; calculated two-nucleon distributions, short-range-correlation(SRC) scaling factors, binding energies from ab initio low-energy nuclear theory.
doi: 10.1088/1361-6471/ab6af7
2017CH55 Phys.Rev.Lett. 119, 262502 (2017) J.-W.Chen, W.Detmold, J.E.Lynn, A.Schwenk Short-Range Correlations and the EMC Effect in Effective Field Theory NUCLEAR STRUCTURE 3H, 3,4He, 9Be, 12C; calculated scaling factors, parameters. Comparison with available data.
doi: 10.1103/PhysRevLett.119.262502
2013CH08 Phys.Rev. C 87, 024910 (2013) J.-W.Chen, J.Deng, H.Dong, Q.Wang Shear and bulk viscosities of a gluon plasma in perturbative QCD: Comparison of different treatments for the gg<->ggg process
doi: 10.1103/PhysRevC.87.024910
2013CH28 Phys.Rev.Lett. 110, 262301 (2013) J.-W.Chen, S.Pu, Q.Wang, X.-N.Wang Berry Curvature and Four-Dimensional Monopoles in the Relativistic Chiral Kinetic Equation
doi: 10.1103/PhysRevLett.110.262301
2012CH43 Phys.Rev. C 86, 054001 (2012) J.-W.Chen, T.-K.Lee, C.-P.Liu, Y.-S.Liu Quark-mass dependence of two-nucleon observables
doi: 10.1103/PhysRevC.86.054001
2009CH20 Phys.Rev. C 79, 044913 (2009) Bulk viscosity of a gas of massless pions
doi: 10.1103/PhysRevC.79.044913
2006AN34 Phys.Rev. D 74, 094013 (2006) Leading chiral corrections to the nucleon generalized parton distributions NUCLEAR STRUCTURE A=1; calculated chiral corrections to generalized parton distributions.
doi: 10.1103/PhysRevD.74.094013
2005CH32 Phys.Rev. C 71, 044321 (2005) Deuteron Compton scattering in effective field theory: Spin-dependent cross sections and asymmetries NUCLEAR REACTIONS 2H(polarized γ, γ), E=30-90 MeV; calculated σ(θ), polarization observables. Effective field theory.
doi: 10.1103/PhysRevC.71.044321
2005CH43 Phys.Lett. B 620, 33 (2005) Deuteron Compton scattering in effective field theory and spin-independent nucleon polarizabilities
doi: 10.1016/j.physletb.2005.06.001
2005CH75 Phys.Rev. C 72, 061001 (2005) J.-W.Chen, T.Inoue, X.Ji, Y.Li Fixing two-nucleon weak-axial coupling L1, A from μ-d capture NUCLEAR REACTIONS 2H(μ-, ν), E at rest; calculated capture σ vs outgoing neutrons relative energy; deduced constraints on weak-axial coupling. Pionless effective field theory.
doi: 10.1103/PhysRevC.72.061001
2004CH14 Nucl.Phys. A735, 441 (2004) Soft pion emission in DVCS
doi: 10.1016/j.nuclphysa.2004.02.005
2004CH58 Phys.Lett. B 603, 6 (2004) Drell-Hearn-Gerasimov sum-rule for the deuteron in nuclear effective field theory NUCLEAR STRUCTURE 2H; calculated sum rule. Effective field theory.
doi: 10.1016/j.physletb.2004.10.016
2004CH63 Phys.Rev.Lett. 93, 242302 (2004) Inequalities for Light Nuclei in the Wigner Symmetry Limit
doi: 10.1103/PhysRevLett.93.242302
2003CH10 Phys.Rev. C 67, 025801 (2003) J.-W.Chen, K.M.Heeger, R.G.H.Robertson Constraining the leading weak axial two-body current by recent solar neutrino flux data
doi: 10.1103/PhysRevC.67.025801
2002CH03 Phys.Rev.Lett. 88, 052003 (2002) Leading Chiral Contributions to the Spin Structure of the Proton NUCLEAR STRUCTURE 1H; calculated chiral contributions to quark and gluon components of proton spin. Heavy-baryon chiral perturbation theory.
doi: 10.1103/PhysRevLett.88.052003
2002CH42 Nucl.Phys. A707, 452 (2002) Matrix Elements of Twist-2 Operators in Quenched Chiral Perturbation Theory
doi: 10.1016/S0375-9474(02)00994-6
2001BU07 Phys.Rev. C63, 035501 (2001) Neutrino-Deuteron Scattering in Effective Field Theory at Next-to-Next-to-Leading Order NUCLEAR REACTIONS 2H(ν, ep), (ν, νp), (ν, e+n), E ≈ 2-20 MeV; calculated σ. Effective field theory.
doi: 10.1103/PhysRevC.63.035501
2001BU29 Phys.Lett. 520B, 87 (2001) Proton-Proton Fusion in Effective Field Theory to Fifth Order NUCLEAR REACTIONS 1H(p, e+ν), E not given; calculated fusion rate, high-order effects. Effective field theory.
doi: 10.1016/S0370-2693(01)01152-2
2001CH14 Phys.Lett. 501B, 209 (2001) Parity-Violating Pion-Nucleon Coupling hπNN(1) from π+-Electroproton Production Near the Threshold NUCLEAR REACTIONS 1H(e, e'π+), E=200, 250 MeV; calculated pion production σ(E, θ), electron-helicity asymmetry.
doi: 10.1016/S0370-2693(01)00100-9
2001CH20 Nucl.Phys. A684, 484c (2001) Neutrino-Deuteron Scattering in Effective Field Theory NUCLEAR REACTIONS 2H(ν, X), E < 20 MeV; calculated deuteron breakup channels σ. Effective field theory.
doi: 10.1016/S0375-9474(01)00450-X
2001CH30 Phys.Rev.Lett. 86, 4239 (2001) Measuring the P-Odd Pion-Nucleon Coupling hπNN(1) in π+-Photoproton Production near Threshold NUCLEAR REACTIONS 1H(polarized γ, π+), E ≈ 150-230 MeV; calculated σ, σ(θ), polarization asymmetry; deduced relation to parity-violating coupling constant.
doi: 10.1103/PhysRevLett.86.4239
2001CH74 Phys.Rev. C64, 055206 (2001) Parity Violation in γ(pol)p Compton Scattering NUCLEAR REACTIONS 1H(polarized γ, γ), E=0-120 MeV; calculated parity-violating helicity asymmetry.
doi: 10.1103/PhysRevC.64.055206
2001CH86 Phys.Lett. 523B, 73 (2001) Large-Nc Quark Distributions in the Delta and Chiral Logarithms in Quark Distributions of the Nucleon NUCLEAR STRUCTURE 1n, 1H; calculated quark distribution features.
doi: 10.1016/S0370-2693(01)01340-5
2000BU20 Nucl.Phys. A675, 575 (2000) Elastic and Inelastic Neutrino-Deuteron Scattering in Effective Field Theory NUCLEAR REACTIONS 2H(ν, nν), (ν-bar, nν-bar), (ν-bar, ne+), E=4-20 MeV; calculated σ. Implications for SNO detector discussed.
doi: 10.1016/S0375-9474(99)00682-X
1999CH20 Nucl.Phys. A653, 375 (1999) Tensor Polarized γ-Deuteron Compton Scattering in Effective Field Theory NUCLEAR REACTIONS 2H(γ, γ'), E < 80 MeV; calculated σ(θ) from polarized target; deduced reaction mechanism features. Effective field theory.
doi: 10.1016/S0375-9474(99)00235-3
1999CH21 Nucl.Phys. A653, 386 (1999) J.-W.Chen, G.Rupak, M.J.Savage Nucleon-Nucleon Effective Field Theory without Pions NUCLEAR REACTIONS 1H(n, γ), E=low; calculated σ, effective range parameters. Effective field theory without pions. NUCLEAR STRUCTURE 2H; calculated form factors. Effective field theory without pions.
doi: 10.1016/S0375-9474(99)00298-5
1999CH31 Phys.Lett. 464B, 1 (1999) Isoscalar M1 and E2 Amplitudes in np → dγ NUCLEAR REACTIONS 1H(n, γ), E=low; calculated isoscaler M1 and E2 amplitudes. NUCLEAR STRUCTURE 2H; calculated quadrupole form factor.
doi: 10.1016/S0370-2693(99)01007-2
1999CH38 Phys.Rev. C60, 065205 (1999) np → dγ for Big-Bang Nucleosynthesis NUCLEAR REACTIONS 1H(n, γ), E(cm) < 1 MeV; 2H(γ, n), E=2.6-9.0 MeV; calculated σ. Pionless nucleon-nucleon effective field theory.
doi: 10.1103/PhysRevC.60.065205
1998CH46 Nucl.Phys. A644, 221 (1998) J.-W.Chen, H.W.Griesshammer, M.J.Savage, R.P.Springer The Polarizability of the Deuteron NUCLEAR STRUCTURE 2H; calculated scalar, tensor polarizabilities. Effective field theory calculations.
doi: 10.1016/S0375-9474(98)00580-6
1998CH47 Nucl.Phys. A644, 245 (1998) J.-W.Chen, H.W.Griesshammer, M.J.Savage, R.P.Springer γ-Deuteron Compton Scattering in Effective Field Theory NUCLEAR REACTIONS 2H(γ, γ'), E=49, 69 MeV; calculated Compton scattering σ(θ). Effective field theory expansion.
doi: 10.1016/S0375-9474(98)00591-0
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