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NSR database version of May 21, 2024.

Search: Author = J.R.Smith

Found 23 matches.

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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
Citations: PlumX Metrics


2005SM06      Phys.Rev. C 72, 022203 (2005)

J.R.Smith, G.A.Miller

Polarized quark distributions in nuclear matter

doi: 10.1103/PhysRevC.72.022203
Citations: PlumX Metrics


2004SM11      Phys.Rev. C 70, 065205 (2004)

J.R.Smith, G.A.Miller

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
Citations: PlumX Metrics


2003SM08      Phys.Rev.Lett. 91, 212301 (2003)

J.R.Smith, G.A.Miller

Chiral Solitons in Nuclei: Saturation, EMC Effect, and Drell-Yan Experiments

doi: 10.1103/PhysRevLett.91.212301
Citations: PlumX Metrics


2002MI02      Phys.Rev. C65, 015211 (2002)

G.A.Miller, J.R.Smith

Return of the EMC Effect

doi: 10.1103/PhysRevC.65.015211
Citations: PlumX Metrics


2002SM06      Phys.Rev. C65, 055206 (2002); Erratum Phys.Rev. C66, 049903 (2002)

J.R.Smith, G.A.Miller

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
Citations: PlumX Metrics


1991SM04      Phys.Rev. C44, 1118 (1991)

J.R.Smith, A.E.Richardson

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0253.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13103.


1972SM03      Nucl.Phys. A186, 161 (1972)

J.R.Smith, S.T.Thornton

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1050.


1972SM04      Can.J.Phys. 50, 783 (1972)

J.R.Smith, S.T.Thornton

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0029.


1972SM05      Nucl.Phys. A187, 433 (1972)

J.R.Smith, S.T.Thornton

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0037.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1509.


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)

J.R.Smith

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11079.


1953CO66      Phys.Rev. 89, 785 (1953)

C.F.Cook, J.R.Smith

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1175.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0008.


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