NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.R.Smith Found 23 matches. 2006DE06 Phys.Rev. C 73, 015204 (2006) W.Detmold, G.A.Miller, J.R.Smith Role of the nuclear vector potential in deep inelastic scattering
doi: 10.1103/PhysRevC.73.015204
2005SM06 Phys.Rev. C 72, 022203 (2005) Polarized quark distributions in nuclear matter
doi: 10.1103/PhysRevC.72.022203
2004SM11 Phys.Rev. C 70, 065205 (2004) Chiral solitons in nuclei: Electromagnetic form factors NUCLEAR STRUCTURE 1H; calculated electromagnetic form factors of bound proton. Chiral quark-soliton model.
doi: 10.1103/PhysRevC.70.065205
2003SM08 Phys.Rev.Lett. 91, 212301 (2003) Chiral Solitons in Nuclei: Saturation, EMC Effect, and Drell-Yan Experiments
doi: 10.1103/PhysRevLett.91.212301
2002MI02 Phys.Rev. C65, 015211 (2002) Return of the EMC Effect
doi: 10.1103/PhysRevC.65.015211
2002SM06 Phys.Rev. C65, 055206 (2002); Erratum Phys.Rev. C66, 049903 (2002) Return of the EMC Effect: Finite nuclei NUCLEAR REACTIONS 16O, 40Ca, 208Pb(e, e'X), E not given; calculated structure function ratios. Comparison with data, possible medium modification of nucleon structure discussed.
doi: 10.1103/PhysRevC.65.055206
1991SM04 Phys.Rev. C44, 1118 (1991) Independent Yields from the Photofission of 232Th, and the Z(p) and Statistical-Dynamic Models NUCLEAR REACTIONS, ICPND 232Th(γ, F)82Br/96Nb/124Sb/126Sb/136Cs, E=11-27 MeV bremsstrahlung; measured residues independent fission yields. Statistical dynamics model, post-fission dynamics.
doi: 10.1103/PhysRevC.44.1118
1990DA13 Hyperfine Interactions 59, 193 (1990) M.P.Dancey, J.Billowes, I.S.Grant, D.E.Evans, J.A.R.Griffith, S.A.Wells, D.A.Eastham, J.Groves, J.R.H.Smith, D.W.L.Tolfree, P.M.Walker Laser Fluorescence on Radio-Active Isotopes Produced in Very Low Yield RADIOACTIVITY 120,121,122,123,124,127mBa [from 92,96,98Mo(32S, xn2p)]; measured hfs; deduced rms radii changes. 127mBa deduced μ, quadrupole moment. Fast ion-photon coincidence, ultra-sensitive laser fluorescence spectroscopy.
1990HO15 Phys.Rev. A41, 5834 (1990) D.Horvath, K.A.Aniol, F.Entezami, D.F.Measday, A.J.Noble, S.Stanislaus, C.J.Virtue, A.S.Clough, D.F.Jackson, J.R.H.Smith, M.Salomon Experimental Study of Pion Capture by Hydrogen Bound in Molecules NUCLEAR REACTIONS 1H(π-, π0), (π-, γ), E at rest; measured σ(E(π)), Eγ, Iγ, En, γγ-coin; deduced pion capture probability. ATOMIC PHYSICS, Mesic-Atoms 1H(π-, π0), (π-, γ), E at rest; measured σ(E(π)), Eγ, Iγ, En, γγ-coin; deduced pion capture probability.
doi: 10.1103/PhysRevA.41.5834
1989PA07 Nucl.Phys. A499, 173 (1989) C.N.Pass, P.M.Evans, A.E.Smith, L.Stuttge, R.R.Betts, J.S.Lilley, D.W.Banes, K.A.Connell, J.Simpson, J.R.Smith, A.N.James, B.R.Fulton Study of Neutron Transfer Reactions at Sub-Coulomb Energies Using a Recoil Separator NUCLEAR REACTIONS 116,118,120,122,124Sn(58Ni, X), (58Ni, 59Ni), E=180-220 MeV; measured σ(θ=180°) vs E, γγ-coin; deduced pickup σ. 123Sn levels deduced neutron pickup strength. One neutron pick-up gamma-ray coincidences. DWBA, semi-classical analyses, sub-barrier fusion calculations.
doi: 10.1016/0375-9474(89)90276-5
1988WE14 Phys.Lett. 211B, 272 (1988) S.A.Wells, D.E.Evans, J.A.R.Griffith, D.A.Eastham, J.Groves, J.R.H.Smith, D.W.L.Tolfree, D.D.Warner, J.Billowes, I.S.Grant, P.M.Walker Fluorescent Atom Coincidence Spectroscopy of Extremely Neutron-Deficient Barium Isotopes RADIOACTIVITY 120,121,122,123,124Ba [from 92,96Mo(32S, xn2p)]; measured hfs, isotope shifts; deduced quadrupole deformation parameter. 120,121,122,123Ba deduced rms charge radii relative to 124Ba. Fluorescent atom coincidence spectroscopy.
doi: 10.1016/0370-2693(88)90902-1
1987BE28 Phys.Rev.Lett. 59, 978 (1987) R.R.Betts, P.M.Evans, C.N.Pass, N.Poffe, A.E.Smith, L.Stuttge, J.S.Lilley, D.W.Banes, K.A.Connell, J.Simpson, J.R.H.Smith, A.N.James, B.R.Fulton Measurement of Subbarrier Transfer Reactions for 58Ni + Sn using a Recoil Mass Separator NUCLEAR REACTIONS 116,118,120,122,124Sn(58Ni, X), E=183-220 MeV; measured σ(E, θ=180°); deduced one-nucleon pickup σ(θ), target mass dependence.
doi: 10.1103/PhysRevLett.59.978
1987EA01 Phys.Rev. C36, 1583 (1987) D.A.Eastham, P.M.Walker, J.R.H.Smith, D.D.Warner, J.A.R.Griffith, D.E.Evans, S.A.Wells, M.J.Fawcett, I.S.Grant Nuclear Charge Radii of Proton-Rich Strontium Isotopes RADIOACTIVITY 78,79,80,81,82,83Sr; measured hfs, isotope shift; deduced μ, rms radii. Atom-photon coincidence laser spectroscopy. NUCLEAR MOMENTS 88,86,87Sr; measured hyperfine structure, isotope shifts; deduced μ, rms radii. Atom-photon coincidence laser spectroscopy.
doi: 10.1103/PhysRevC.36.1583
1986EA01 J.Phys.(London) G12, L205 (1986) D.A.Eastham, P.M.Walker, J.R.H.Smith, J.A.R.Griffith, D.E.Evans, S.A.Wells, M.J.Fawcett, I.S.Grant Optical Isotope Shifts of 80,82Sr from Coincidence Laser Spectroscopy NUCLEAR MOMENTS 80,82Sr; measured isotope shifts. 84,82,80Sr deduced rms charge radii differences. Ultra sensitive laser fluorescence technique.
doi: 10.1088/0305-4616/12/9/003
1986RI07 Nucl.Sci.Eng. 94, 413 (1986) A.E.Richardson, H.L.Wright, J.L.Meason, J.R.Smith Mass Distribution in the Fission of 232Th by Degraded-Fission-Spectrum Neutrons NUCLEAR REACTIONS 232Th(n, F)83Se/84Br/85Kr/85mKr/87Kr/88Kr/91Sr/91Y/91mY/92Sr/92Y/94Y/95Nb/97Nb/97mNb/99Mo/99Tc/99mTc/129Sb/130Sb/131I/132I/133I/134I/135I/132Te/135Xe/135mXe/138Cs/139Ba/140La/142La/141Ce/143Ce/146Pr/147Nd/149Nd, E=fission spectrum; measured residual yields, fission fragment mass distribution. Degraded fission spectrum, activation technique.
doi: 10.13182/NSE86-A18351
1972SM03 Nucl.Phys. A186, 161 (1972) Measurements of 3H(p, n)3He Neutron Polarizations for E = 1.5 to 5.0 Mev NUCLEAR REACTIONS 3H(p, n) , Ep=1.50, 1.75, 1.90, 2.26, 2.46, 2.70, 3.12, 3.50, 3.90, 4.41, 5.00 MeV; measured neutron P(En, θ); calculated Legendre polynomial expansion coefficients for σ(θ), P(θ)σ(θ). Gas target.
doi: 10.1016/0375-9474(72)90132-7
1972SM04 Can.J.Phys. 50, 783 (1972) Measurements of D(d, n)3He Neutron Polarizations for Deuteron Energies from 0.87 to 5.00 MeV NUCLEAR REACTIONS 2H(d, n), E=0.87-5.00 MeV; measured P(n)(E;θ); deduced Legendre coefficients.
doi: 10.1139/p72-111
1972SM05 Nucl.Phys. A187, 433 (1972) Measurements of 3H(d, n)4He Neutron Polarizations for E = 1.0 to 5.0 Mev NUCLEAR REACTIONS 3H(d, n), Ed=1.00, 1.50, 2.00, 3.00, 4.00, 4.35, 5.00 MeV; measured neutronp(En, θ). A contour map of P(θ) was produced from Legendre polynomial fits. Gas target.
doi: 10.1016/0375-9474(72)90587-8
1971TH07 Nucl.Phys. A169, 131 (1971) S.T.Thornton, C.L.Morris, J.R.Smith, R.P.Fogel 7Li(p, n)7Be Neutron Polarization Measurements for E = 3.0 to 5.5 MeV NUCLEAR REACTIONS 7Li(p, n), Ep=3.0, 3.5, 4.0, 4.5, 5.0, 5.5 MeV; measured neutron P(En, θ). Contour maps of P(θ), P2(θ)σ(θ) are produced from Legendre polynomial fits.
doi: 10.1016/0375-9474(71)90567-7
1958RE05 Bull.Am.Phys.Soc. 3, No.1, 6, A5 (1958) R.B.Regier, W.H.Burgus, J.R.Smith, M.S.Moore Neutron Energy Dependent Mass Distribution in U233 Fission
1954SM97 Phys.Rev. 95, 730 (1954) Scattering Of 14.1-Mev Neutrons In Helium, Hydrogen And Nitrogen NUCLEAR REACTIONS 1H(n, n), 4He(n, n), N(n, n), N(n, n'), E=14.1 MeV; measured products, Eπ, Iπ; deduced σ(θ), σ, σ(E). Data were imported from EXFOR entry 11079.
doi: 10.1103/PhysRev.95.730
1953CO66 Phys.Rev. 89, 785 (1953) Cross section for the reaction D(d, p)3H NUCLEAR REACTIONS 2H(d, p), E=48.8-102 keV; measured products, 3H, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry A1175.
doi: 10.1103/PhysRev.89.785
1952CO35 Phys.Rev. 88, 468 (1952) J.P.Conner, T.W.Bonner, J.R.Smith A Study of the H3(d, n)He4 Reaction
doi: 10.1103/PhysRev.88.468
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