NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = E.Henley Found 62 matches. 2014BU11 Few-Body Systems 55, 749 (2014) Three-Quark Currents and Baryon Spin
doi: 10.1007/s00601-014-0864-9
2011AL22 Eur.Phys.J. A 47, 140 (2011) M.Altenbuchinger, Ph.Hagler, W.Weise, E.M.Henley Spin structure of the nucleon: QCD evolution, lattice results and models NUCLEAR STRUCTURE 1H; calculated spin structure using lattice QCD with different potentials.
doi: 10.1140/epja/i2011-11140-2
2011KI05 Eur.Phys.J. A 47, 8 (2011) QCD: The Λ(1405) as a hybrid
doi: 10.1140/epja/i2011-11008-5
2010HE21 Nucl.Phys. A842, 72 (2010) A simple quark model for γp → K+Λ0
doi: 10.1016/j.nuclphysa.2010.04.015
2010HE22 Nucl.Phys. A844, 185c (2010) Some symmetries in nuclear physics
doi: 10.1016/j.nuclphysa.2010.05.033
2008BU09 Eur.Phys.J. A 35, 267 (2008) Baryon octupole moments
doi: 10.1140/epja/i2007-10565-4
2006HE15 Phys.Rev. D 73, 094004 (2006) Ultrahigh energy neutrino-nucleon scattering and parton distributions at small x NUCLEAR REACTIONS 1H(ν, X), E=high; calculated σ, sensitivity to parton distributions.
doi: 10.1103/PhysRevD.73.094004
2005AL12 Phys.Lett. B 611, 111 (2005) Parton distributions in the proton and pion
doi: 10.1016/j.physletb.2005.02.033
2005CA12 Eur.Phys.J. A 24, Supplement 2, 103 (2005) Corrections to the nuclear axial vector coupling in a nuclear medium
doi: 10.1140/epjad/s2005-04-023-1
2005CA55 Int.J.Mod.Phys. E14, 1017 (2005) Corrections to the nuclear axial vector coupling in a nuclear medium
doi: 10.1142/S0218301305003685
2005HE06 Nucl.Phys. B(Proc.Supp.) S143, 497 (2005) Ultra-High Energy Neutrino-Nucleon Scattering NUCLEAR REACTIONS 1n, 1H(ν, X), E > 1000 TeV; calculated total σ.
doi: 10.1016/j.nuclphysbps.2005.01.162
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
2001BU03 Phys.Rev. C63, 015202 (2001) Intrinsic Quadrupole Moment of the Nucleon NUCLEAR STRUCTURE 1H; calculated intrinsic quadrupole moment for proton, Δ resonance; deduced deformation.
doi: 10.1103/PhysRevC.63.015202
2001HE07 Phys.Lett. 502B, 99 (2001) Coordinate Space Distributions of Antiquark Flavor Asymmetries in the Proton NUCLEAR STRUCTURE 1H; calculated antiquark distributions.
doi: 10.1016/S0370-2693(01)00190-3
2000AL14 Nucl.Phys. A663-664, 301c (2000) Light Quark Distributions in the Proton Sea NUCLEAR STRUCTURE 1H; calculated light antiquark asymmetry. Meson cloud model, comparison with data.
doi: 10.1016/S0375-9474(99)00600-4
1999HE04 Rev.Mod.Phys. 71, S205 (1999) Nuclear Physics at the End of the Century
doi: 10.1103/RevModPhys.71.S205
1998AD12 Rev.Mod.Phys. 70, 1265 (1998) E.G.Adelberger, S.M.Austin, J.B.Bahcall, A.B.Balantekin, G.Bogaert, L.S.Brown, L.Buchmann, F.E.Cecil, A.E.Champagne, L.de Braeckeleer, C.A.Duba, S.R.Elliott, S.J.Freedom, M.Gai, G.Goldring, C.R.Gould, A.Gruzinov, W.C.Haxton, K.M.Heeger, E.Henley, C.W.Johnson, M.Kamionkowski, R.W.Kavanagh, S.E.Koonin, K.Kubodera, K.Langanke, T.Motobayashi, V.Pandharipande, P.Parker, R.G.H.Robertson, C.Rolfs, R.F.Sawyer, N.Shaviv, T.D.Shoppa, K.A.Snover, E.Swanson, R.E.Tribble, S.Turck-Chieze, J.F.Wilkerson Solar Fusion Cross Sections NUCLEAR REACTIONS 7Be, 12,13C, 15N, 16,17,18O(p, γ), 14,15N, 17,18O(p, α), 7Li(d, p), 3He(p, e+), (α, γ), (3He, 2p), 1H(p, e+), E=low; compiled, analyzed S-factor data, calculations; deduced implications for solar neutrino flux calculations.
doi: 10.1103/RevModPhys.70.1265
1998HE27 Acta Phys.Pol. B29, 2459 (1998) Flavor Asymmetry in Hyperons and Drell-Yan Processes
1997ME06 Phys.Rev. C55, 3093 (1997) Isospin Breaking in the Pion-Nucleon Coupling from QCD Sum Rules
doi: 10.1103/PhysRevC.55.3093
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
1995CH18 Phys.Lett. 343B, 7 (1995) C.-T.Chan, E.M.Henley, T.Meissner π-(Eta) Mixing from QCD Sum Rules
doi: 10.1016/0370-2693(94)01461-K
1995YI01 Nucl.Phys. A585, 463 (1995) Time-Reversal Invariance in the β-Decays of A = 8 Nuclei RADIOACTIVITY 8B(β+); 8Li(β-); calculated α-particle spectra following β-decay. Final state interactions included, R-matrix, parameters from 4He(α, α) analysis. NUCLEAR REACTIONS 4He(α, α), E=0-25 MeV; analyzed phase shifts vs E; deduced R-matrix parameters.
doi: 10.1016/0375-9474(94)00720-8
1994AL34 Yad.Fiz. 57, No 9, 1678 (1994); Phys.Atomic Nuclei 57, 1608 (1994) M.A.Alberg, E.M.Henley, L.Wilets, P.D.Kunz A Quark Model of (Lambda-bar)(Lambda) Production in (p-bar)p Interactions NUCLEAR REACTIONS 1H(p-bar, X), E=threshold-1695 MeV/c; analyzed σ, σ(θ), polarization observables data following (lambda-bar)(lambda) production. Quark model.
1994AL51 Nuovo Cim. 107A, 2483 (1994) M.A.Alberg, E.M.Henley, L.Wilets, P.D.Kunz A Quark Model of (Lambda-bar)Lambda Production in (p-bar)p Interactions NUCLEAR REACTIONS 1H(p-bar, X), E=threshold-1.92 GeV/c; calculated σ(θ) for (lambda-bar)(lambda) production. DWBA.
doi: 10.1007/BF02734020
1994KO08 Phys.Rev. C49, 2219 (1994) Electromagnetic Gauge Invariance of Chiral Hybrid Quark Models NUCLEAR STRUCTURE 1H; calculated π+ cloud contribution to magnetic form factor; deduced chiral hybrid quark models electromagnetic gauge invariance features.
doi: 10.1103/PhysRevC.49.2219
1993AL16 Nucl.Phys. A560, 365 (1993) M.A.Alberg, E.M.Henley, L.Wilets, P.D.Kunz A Quark Model of Antilambda-Lambda Production in (p-bar)p Interactions NUCLEAR REACTIONS 1H(p-bar, X), E at 1436-1695 MeV/c; calculated (lambda)(lambda-bar) production σ(θ), asymmetry; analyzed σ(θ), polarization, spin correlation coefficients data; deduced model parameters. Quark model, DWBA approach.
doi: 10.1016/0375-9474(93)90102-4
1993HE16 Czech.J.Phys. B43, 289 (1993) Discrete Space-Time Symmetries
doi: 10.1007/BF01589848
1992HE12 Phys.Lett. 289B, 223 (1992) First Forbidden β-Decays as a Probe of T-Odd Nuclear Forces RADIOACTIVITY 11Be, 17N(β-); 18Ne(β+); 19Ne(β+), (EC); 36K(β+); 39Cl(β-); 107Cd(β+)(EC); 154Eu(β-), (EC); 169Hf(EC), (β+); 231Th(β-); 235Pa(β-); calculated square root of branching ratio for decay to final levels; deduced enhancements due to level mixing caused by T-odd forces.
doi: 10.1016/0370-2693(92)91209-R
1992KO12 Phys.Lett. 288B, 11 (1992) W.Koepf, E.M.Henley, S.J.Pollock Strangeness Matrix Elements in the Nucleon NUCLEAR STRUCTURE 1n, 1H; calculated μ, rms radii ratio; deduced strangeness content of proton. Relativistic meson loop, nonrelativistic quark, extended cloudy bag models.
doi: 10.1016/0370-2693(92)91947-8
1992YI01 Phys.Rev. C45, 1982 (1992) S.Ying, W.C.Haxton, E.M.Henley Charged- and Neutral-Current Solar-Neutrino Cross Sections for Heavy-Water Cherenkov Detectors NUCLEAR REACTIONS 2H(ν, X), E=3.25-160 MeV; calculated charged, neutral current σ. Bonn, Paris, Hamada-Johnson potentials.
doi: 10.1103/PhysRevC.45.1982
1991FR06 Nucl.Phys. A533, 617 (1991) T.Frederico, E.M.Henley, G.A.Miller Parity Violation in Elastic Electron-Deuteron Scattering. Light-Front Dynamics NUCLEAR REACTIONS 2H(polarized e, e), E=0.3-1.9 GeV; calculated recoil deuteron parity violating asymmetry; deduced nucleon strangeness role.
doi: 10.1016/0375-9474(91)90536-F
1990HE26 Nucl.Phys. A518, 207 (1990) The Proton Charge Form Factors and the Neutron-Proton Mass Difference NUCLEAR STRUCTURE 1n, 1H; analyzed proton charge form factor; deduced gluon exchange, electromagnetic, kinetic energy contributions.
doi: 10.1016/0375-9474(90)90546-X
1989HA22 Phys.Rev.Lett. 63, 949 (1989) W.C.Haxton, E.M.Henley, M.J.Musolf Nucleon and Nuclear Anapole Moments NUCLEAR STRUCTURE 19F, 133Cs; calculated one-body, polarization, exchange-current contribution to the anapole matrix element. Shell model.
doi: 10.1103/PhysRevLett.63.949
1989HE09 Phys.Rev.Lett. 62, 2586 (1989) Nambu-Jona-Lasinio Model and Charge Independence NUCLEAR STRUCTURE A=16, 40; calculated average nucleon masses, neutron-proton mass differences. Nambu-Jona-Lasinio model.
doi: 10.1103/PhysRevLett.62.2586
1989HE26 Phys.Lett. 231B, 213 (1989) Chiral Symmetry, Constituent Quarks and Quasi-Elastic Electron-Nucleus Scattering NUCLEAR REACTIONS 12C, 40Ca, 56Fe(e, e'), E not given; calculated quasielastic longitudinal, transverse structure functions; deduced chiral symmetry breaking role. Nambu-Jona-Lasinio model.
doi: 10.1016/0370-2693(89)90201-3
1988HE10 Nucl.Phys. A483, 596 (1988) Parity Nonconservation in Proton-Proton Scattering at 6 GeV/c NUCLEAR REACTIONS 1H(polarized p, p), E at 6 GeV/c; analyzed data; deduced parity violating asymmetry.
doi: 10.1016/0375-9474(88)90085-1
1988SH31 Phys.Rev. C38, 1584 (1988) Shuqian Ying, E.M.Henley, G.A.Miller Deuteron Photodisintegration NUCLEAR REACTIONS 2H(γ, p), E ≈ 10-120 MeV; calculated σ(θ) vs E. Relativistic, pion exchange, isobar correction effects.
doi: 10.1103/PhysRevC.38.1584
1986BR30 Phys.Rev. C34, 1779 (1986) K.Brauer, E.M.Henley, G.A.Miller Isospin Nonconservation in Nucleon-Nucleon Scattering by a Color Force NUCLEAR REACTIONS 1H(polarized n, n), 1n(polarized p, p), E=477 MeV; calculated polarization difference; deduced gluon exchange contribution. Nonrelativistic quark potential model.
doi: 10.1103/PhysRevC.34.1779
1983HO02 Phys.Rev. C27, 277 (1983) P.Hoodbhoy, R.A.Freedman, G.A.Miller, E.M.Henley Pion-Nucleus Charge-Exchange Reactions with Isobar Dynamics NUCLEAR REACTIONS 18O(π+, π-), (π+, π0), E=164 MeV; calculated σ(θ). Optical model, isobar dynamics.
doi: 10.1103/PhysRevC.27.277
1983KL05 Phys.Rev. C27, 2529 (1983) W.M.Kloet, B.F.Gibson, G.J.Stephenson, Jr., E.M.Henley Parity Nonconserving Asymmetry in Neutron-Deuteron and Proton-Deuteron Scattering NUCLEAR REACTIONS 2H(polarized p, p), (polarized n, p), E=14-40 MeV; calculated σ(E), parity nonconserving asymmetry.
doi: 10.1103/PhysRevC.27.2529
1982FR17 Nucl.Phys. A389, 457 (1982) R.A.Freedman, G.A.Miller, E.M.Henley Isobar Dynamics and Pion-Nucleus Elastic Scattering NUCLEAR REACTIONS 16O, 40,48Ca, 208Pb(π+, π+), E=114-240 MeV; calculated σ(θ). Isobar dynamics.
doi: 10.1016/0375-9474(82)90425-0
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
1981FR14 Phys.Lett. 103B, 397 (1981) R.A.Freedman, G.A.Miller, E.M.Henley Pion-Nucleus Scattering and Systematics of the Delta-Nucleus Potential NUCLEAR REACTIONS 16O, 40Ca(π+, π+), E=163 MeV; 28Si(π+, π+), E=162 MeV; calculated σ(θ); deduced isobar-nucleus potential systematics.
doi: 10.1016/0370-2693(81)90068-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
1981HW01 Nucl.Phys. A356, 365 (1981) Parity Violation: Radiative pion capture in hydrogen NUCLEAR REACTIONS 1H(π-, γ), E at rest; calculated γ- CP; deduced effect of Δ-resonance, ρ-meson on parity-violating pion-nucleon-nucleon coupling constant. Light vector meson, Δ-resonance contributions, Chew-Goldberger-Low-Nambu transition amplitude.
doi: 10.1016/0375-9474(81)90195-0
1981HW02 Ann.Phys.(New York) 137, 378 (1981) W-Y.P.Hwang, E.M.Henley, G.A.Miller Parity Violation in Electron-Deuteron Scattering. II. Break-Up Channels NUCLEAR REACTIONS 2H(e, e'), E=5-50, 100-500 MeV; calculated σ(θ(e'), E(e')), asymmetry; deduced parity violation effect energy dependence. Impulse approximation, gauge invariance, meson exchange currents.
doi: 10.1016/0003-4916(81)90201-3
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
1980HA41 Phys.Rev.Lett. 45, 1677 (1980) W.C.Haxton, B.F.Gibson, E.M.Henley Parity Nonconservation in 18F, 19F, and 21Ne NUCLEAR STRUCTURE 18,19F, 21Ne; calculated γ-circular polarization, γ-asymmetry; deduced parity nonconserving interaction matrix elements. Weinberg-Salam model.
doi: 10.1103/PhysRevLett.45.1677
1978AL24 Nucl.Phys. A306, 447 (1978) M.A.Alberg, E.M.Henley, G.A.Miller, J.F.Walker Field-Theory Treatment of the pp → dπ+ Reaction NUCLEAR REACTIONS 1H(p, π+d), E=400-800 MeV; calculated σ(E).
doi: 10.1016/0375-9474(78)90474-8
1977KL07 Phys.Rev.Lett. 39, 1392 (1977) W.M.Kloet, B.F.Gibson, G.J.Stephenson, Jr., E.M.Henley Parity-Nonconserving Asymmetry in n-d Scattering NUCLEAR REACTIONS 2H(polarized n, X), E=14.4 MeV; calculated weak parity-nonconserving asymmetry in total σ.
doi: 10.1103/PhysRevLett.39.1392
1976AL03 Ann.Phys.(New York) 96, 43 (1976) M.Alberg, E.M.Henley, L.Wilets Theory of Kaonic Atoms ATOMIC PHYSICS, Mesic-Atoms 10,11B, 12C, 31P, 32S, 35Cl, 27Al, 28Si, Ni, Cu; analyzed theory of kaonic atoms.
doi: 10.1016/0003-4916(76)90111-1
1976HE01 Nucl.Phys. A256, 349 (1976) E.M.Henley, F.R.Krejs, L.Wilets Nuclear Polarization in Muonic He Ions NUCLEAR STRUCTURE 3,4He; calculated polarization effects in muonic atoms.
doi: 10.1016/0375-9474(76)90377-8
1974HO14 Nucl.Phys. A225, 205 (1974) Highly Inelastic Scattering of α-Particles from 208Pb NUCLEAR REACTIONS 208Pb(α, α'), 208Pb(α, 5He), E=65 MeV; calculated σ(Eα', θ), σ(E(5He), θ).
doi: 10.1016/0375-9474(74)90539-9
1972HE16 Nucl.Phys. A189, 632 (1972) Charge-Symmetry Breaking and n-n Scattering Lengths
doi: 10.1016/0375-9474(72)90318-1
1971CH50 Phys.Rev.Lett. 27, 1657 (1971) Possible Explanation for Gross-Structure Observations in the Direct Scattering of Helium Ions NUCLEAR REACTIONS 208Pb(α, α'n), (α, α'p), E=65 MeV; calculated σ(Eα').
doi: 10.1103/PhysRevLett.27.1657
1969HE12 Phys.Rev.Letters 23, 941 (1969) E.M.Henley, T.E.Keliher, D.U.L.Yu Parity-Forbidden Decay of the 8.88-MeV 16O State RADIOACTIVITY 16O; calculated α-width for 8.88-MeV state.
doi: 10.1103/PhysRevLett.23.941
1965HE03 Bull.Am.Phys.Soc. 10, No.1, 51, DC6 (1965) He3(d, t)2p Reaction NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
1964HE06 Phys.Rev. 133, B1445 (1964) Double Stripping: (He3, n) Reaction NUCLEAR STRUCTURE 122Te, 12C, 60Zn, 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.133.B1445
1960HE04 Phys.Rev. 118, 248 (1960) Decay of Be9* (2.43-MeV State) NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.118.228
1958BL57 Phys.Rev. 112, 2029 (1958) Inelastic Scattering from Light Nuclei--the Alpha-Particle Model for Be9
doi: 10.1103/PhysRev.112.2029
1958HE59 Revs.Modern Phys. 30, 438 (1958) Nuclear Radii from Mesonic Atoms
doi: 10.1103/RevModPhys.30.438
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