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NSR database version of May 24, 2024.

Search: Author = T.B.Clegg

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2023CO08      Nucl.Instrum.Methods Phys.Res. A1056, 168654 (2023)

A.L.Cooper, S.Hunt, L.Downen, K.Setoodehnia, F.Portillo, C.Marshall, T.B.Clegg, A.E.Champagne, R.Longland

Correlated characterization of 20Ne-implanted targets using nuclear reaction analysis, Rutherford backscattering spectrometry, and ion transport modeling

NUCLEAR REACTIONS 20Ne(p, γ), E=1169 keV; 20Ne(α, α), E=2 MeV; measured reaction products, Eγ, Iγ; deduced resonance parameters, yields. The model FN tandem Van de Graaff accelerator at TUNL.

doi: 10.1016/j.nima.2023.168654
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2023CO09      Nucl.Instrum.Methods Phys.Res. A1056, 168648 (2023)

A.L.Cooper, S.Hunt, L.Downen, K.Setoodehnia, F.Portillo, C.Marshall, T.B.Clegg, A.E.Champagne, R.Longland

252Cf yield calibration method for nuclear material accountancy and safeguards practitioners

RADIOACTIVITY 252Cf(SF); measured decay products, En, In; deduced neutron yields using passive neutron correlation counting (PNCC). The neutron source used in this evaluation was previously certified by the National Institutes of Science and Technology (NIST), which provides a reference for the accuracy of the PNCC method.

doi: 10.1016/j.nima.2023.168648
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2022DO04      Phys.Rev. C 105, 055804 (2022)

L.N.Downen, C.Iliadis, A.E.Champagne, T.B.Clegg, A.Coc, J.Dermigny

Thermonuclear reaction rate of 29Si(p, γ)30P

NUCLEAR REACTIONS 29Si(p, γ), E(cm)=200-420 keV; measured Eγ, Iγ, γγ-coin; deduced resonance energies, resonance strengths. 30P; deduced levels, J, π, branching ratios. 29Si(p, γ), T=0.01-5.0 GK; deduced total thermonuclear reaction rates. Investigated the influence of possibly unobserved resonances on the reaction rates. Comparison to other experimental data. HPGe detector surrounded by a 16-segment NaI(Tl) annulus comprising LENA γγ-coincidence spectrometer at TUNL.

doi: 10.1103/PhysRevC.105.055804
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2769. Data from this article have been entered in the XUNDL database. For more information, click here.


2013CE04      Phys.Rev. C 88, 065806 (2013)

J.M.Cesaratto, A.E.Champagne, M.Q.Buckner, T.B.Clegg, S.Daigle, C.Howard, C.Iliadis, R.Longland, J.R.Newton, B.M.Oginni

Measurement of the Erc.m.=138 keV resonance in the 23Na(p, γ)24Mg reaction and the abundance of sodium in AGB stars

NUCLEAR REACTIONS 23Na(p, γ)24Mg, E<500 keV; measured Eγ, Iγ, on resonance γγ-coin spectra using ECRIS ion source at LENA-TUNL accelerator facility; deduced upper limit on the strength of the 138-keV proton resonance, probability density of the final 23Na abundance, (p, α)/(p, γ) reaction rate ratio, correlations between the final abundance of 23Na in AGB stars and the rate-variation factor. 23Na(p, α)20Ne, E at T9=0.010-10.0; deduced reaction rates for 138-keV resonance. Performed one-zone post-processing nucleosynthesis calculations.

doi: 10.1103/PhysRevC.88.065806
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2076.


2012AR01      Phys.Rev. C 85, 044605 (2012)

C.W.Arnold, T.B.Clegg, C.Iliadis, H.J.Karwowski, G.C.Rich, J.R.Tompkins, C.R.Howell

Cross-section measurement of 9Be(γ, n)8Be and implications for α+α+n → 9Be in the r process

NUCLEAR REACTIONS 9Be(γ, n)8Be, E=1.5-5.2 MeV; measured neutron spectra, Eγ, σ(E) using HIγS facility at TUNL. 9Be; deduced resonance energies, neutron and gamma widths, B(E1), B(M1), neutron branching ratios. Deduced astrophysical reaction rate for 4He(αn, γ)9Be reaction for r-process nucleosynthesis sites. Comparison with previous studies using (γ, n) and (e, e') reactions.

doi: 10.1103/PhysRevC.85.044605
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0171. Data from this article have been entered in the XUNDL database. For more information, click here.


2012BU16      Phys.Rev. C 86, 065804 (2012)

M.Q.Buckner, C.Iliadis, J.M.Cesaratto, C.Howard, T.B.Clegg, A.E.Champagne, S.Daigle

Thermonuclear reaction rate of 18O(p, γ)19F

NUCLEAR REACTIONS 18O(p, γ)19F, E=95 keV; measured Eγ, Iγ, γγ-coin; deduced resonance strength, direct capture S factor using LENA facility. Improved thermonuclear reaction rates.

doi: 10.1103/PhysRevC.86.065804
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1964. Data from this article have been entered in the XUNDL database. For more information, click here.


2012CO11      Phys.Rev. C 85, 054004 (2012)

A.H.Couture, T.B.Clegg, S.Tajima, C.R.Howell, B.Fallin, J.H.Esterline, A.S.Crowell, B.J.Crowe, D.M.Markoff, L.C.Cumberbatch, R.S.Pedroni, H.Witala

Cross-section measurements of 2H(n, np)n in symmetric star configurations

NUCLEAR REACTIONS 2H(n, np), E=16, 19 MeV; measured particle spectra, time-of-flight, np-coin, σ in space-star (SST) and coplanar star (CST) neutron-deuteron breakup configurations. Comparison with Monte Carlo simulations based on rigorous three-nucleon Faddeev calculations. Discussed discrepancies between data and theory; deficiencies in theoretical treatment of three-nucleon forces or in knowledge of the neutron-neutron 1S0 force.

doi: 10.1103/PhysRevC.85.054004
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14337.


2010DA18      Phys.Rev. C 82, 034002 (2010)

T.V.Daniels, C.W.Arnold, J.M.Cesaratto, T.B.Clegg, A.H.Couture, H.J.Karwowski, T.Katabuchi

Spin-correlation coefficients and phase-shift analysis for p+3He elastic scattering

NUCLEAR REACTIONS 3He(polarized p, p), E=2-6 MeV; measured Ep, Ip, analyzing powers; deduced phase shifts, spin-correlation coefficients using polarized 3He target. Comparison with theoretical calculations using realistic nucleon-nucleon potential models.

doi: 10.1103/PhysRevC.82.034002
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1818.


1992BO14      Phys.Rev. C45, 2824 (1992)

J.E.Bowsher, T.B.Clegg, H.J.Karwowski, E.J.Ludwig, W.J.Thompson, J.A.Tostevin

Effects of 6Li Excitation in 64Zn(d(pol), 6Li)60Ni at Low Energies

NUCLEAR REACTIONS 64Zn(polarized d, 6Li), E=16.4 MeV; measured σ(θ), analyzing power vs θ; deduced 6Li levels role in reaction mechanism, model parameters. Vector, tensor polarized beam. Finite-range, coupled-channel Born approximation analysis.

doi: 10.1103/PhysRevC.45.2824
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1416.


1992DA01      Phys.Rev.Lett. 68, 1112 (1992)

R.K.Das, T.B.Clegg, H.J.Karwowski, E.J.Ludwig

Precise Determination of Triton D-State Parameters Using Transfer Reactions at Sub-Coulomb Energies

NUCLEAR REACTIONS 95Mo(polarized d, t), E=7 MeV; 119Sn(polarized d, t), E=6.7 MeV; 149Sm(polarized d, t), E=8 MeV; measured σ(θ), tensor analyzing power vs θ. 3H deduced D-state parameters. Exact finite-range DWBA.

doi: 10.1103/PhysRevLett.68.1112
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1428.


1992LU04      Phys.Rev.Lett. 69, 2448 (1992)

E.J.Ludwig, R.K.Das, T.B.Clegg, H.J.Karwowski

Ludwig et al. Reply:

doi: 10.1103/PhysRevLett.69.2448
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1992WI13      Nucl.Phys. A549, 223 (1992)

J.F.Wilkerson, T.M.Mooney, R.E.Fauber, T.B.Clegg, H.J.Karwowski, E.J.Ludwig, W.J.Thompson

Isospin-Nonconserving Particle Decays in Light Nuclei

NUCLEAR REACTIONS 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar(polarized p, p), E ≈ resonance; 23Na, 31P(polarized p, p), (polarized p, α), 24Mg, 28Si(α, α), 20Ne(polarized p, p), E=6.4-7.7 MeV; measured σ(θ, E), analyzing power vs E, θ; deduced σ(E). 13N, 17F, 24Na, 25Al, 29P, 33S, 37K, 24Mg, 32S, 28Si deduced resonance parameters, isospin-nonconservation probabilities. Enriched targets, ion-implanted targets, polarized and unpolarized beams.

doi: 10.1016/0375-9474(92)90041-H
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0066.


1991BH02      Nucl.Phys. A526, 36 (1991)

C.M.Bhat, E.J.Ludwig, T.B.Clegg, H.J.Karwowski

A Determination of the Asymptotic D- to S-State Ratio for 3He

NUCLEAR REACTIONS 32S(polarized d, 3He), E=16 MeV; measured σ(θ), tensor analyzing power vs θ. 3He deduced D-state. Finite-range DWBA analysis.

doi: 10.1016/0375-9474(91)90296-I
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1557.


1991VA14      Phys.Rep. 201, 57 (1991)

R.L.Varner, W.J.Thompson, T.L.McAbee, E.J.Ludwig, T.B.Clegg

A Global Nucleon Optical Model Potenital

doi: 10.1016/0370-1573(91)90039-O
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1990LU10      J.Phys.(Paris), Colloq.C-6, 439 (1990)

E.J.Ludwig, C.M.Bhat, T.B.Clegg, E.R.Crosson, H.J.Karwowski, G.Graw, P.Schiemenz, R.Hertenberger, H.Kader, D.Hofer, M.Bisenberger, A.M.Eiro, F.D.Santos

D-State Parameter Determinations for 3He and 4He

NUCLEAR REACTIONS 32S(polarized d, 3He), E=16 MeV; 58Ni(polarized d, α), E=22 MeV; measured σ(θ), analyzing power vs θ. 3,4He deduced asymptotic D- to S-state ratio, D2 parameter.


1989AB17      Nucl.Instrum.Methods Phys.Res. A284, 409 (1989)

D.J.Abbott, H.J.Karwowski, T.B.Clegg, E.J.Ludwig

A Deuteron Polarimeter for Polarization Transfer Experiments

NUCLEAR REACTIONS 3He(polarized d, p), E=5-12 MeV; measured vector, tensor analyzing powers vs E. Deuteron polarimeter calibration.

doi: 10.1016/0168-9002(89)90310-0
Citations: PlumX Metrics


1989CL08      Phys.Rev. C40, 2527 (1989)

T.B.Clegg, G.Haouat, J.P.Delaroche, Ch.Lagrange, J.Chardine, M.T.McEllistrem, S.E.Hicks, G.R.Shen

Dynamics of Collective Excitations in 190,192Os and 194Pt Observed by 8 MeV Neutron Scattering

NUCLEAR REACTIONS 190,192Os, 194Pt(n, n), (n, n'), E=8 MeV; measured σ(θ); deduced model parameters. 190Os, 194Pt deduced deformation features.

doi: 10.1103/PhysRevC.40.2527
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1988BH02      Phys.Rev. C37, 1358 (1988)

C.M.Bhat, T.B.Clegg, H.J.Karwowski, E.J.Ludwig

D-State Amplitudes of Three-Nucleon Systems using Single-Nucleon Transfer Reactions

NUCLEAR REACTIONS 31P(polarized d, 3He), 31P(polarized d, t), E ≈ 16 MeV; measured absolute σ(θ), tensor analyzing power vs θ. 3He, 3H deduced D-state amplitudes. Finite-range DWBA analysis. Enriched target.

doi: 10.1103/PhysRevC.37.1358
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1988BH09      Phys.Rev. C38, 1537 (1988)

C.M.Bhat, J.E.Bowsher, T.B.Clegg, H.J.Karwowski, E.J.Ludwig, B.A.Brown

Single-Nucleon Pickup Spectroscopic Factors for Levels in 30Si and 30P and the D State of Three-Nucleon Systems

NUCLEAR REACTIONS 31P(polarized d, 3He), (polarized d, t), (polarized d, d), E=16 MeV; measured σ(θ), vector, tensor analyzing powers vs θ; deduced model parameters. 30Si, 30P levels deduced spectroscopic factors.

doi: 10.1103/PhysRevC.38.1537
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1987AB05      Phys.Rev. C35, 2028 (1987)

D.J.Abbott, T.B.Clegg, J.P.Delaroche

Polarized Proton Scattering from 116,120,124Sn at 16 MeV

NUCLEAR REACTIONS 116,120,124Sn(polarized p, p), (polarized p, p'), E=16 MeV; measured σ(θ), A(θ); deduced deformation lengths, optical model parameters. Enriched targets. Coupled-channels analyses.

doi: 10.1103/PhysRevC.35.2028
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1987VA01      Phys.Lett. 185B, 6 (1987)

R.L.Varner, T.B.Clegg, T.L.McAbee, W.J.Thompson

Global Parameterization of the Nucleon-Nucleus Scattering Potential

NUCLEAR REACTIONS 40Ca, 54Fe, 58,60Ni, 65Cu, 116,120Sn, 208Pb(n, n), (polarized n, n), E=10-26 MeV; 114,112Cd, 116,118,120,122Sn(p, p), (polarized p, p), E=16-65 MeV; 60,62,64Ni, 89Y, 90Zr(p, p), (polarized p, p), E=65 MeV; analyzed σ(θ), analyzing power data; deduced new optical potential parameters.

doi: 10.1016/0370-2693(87)91518-8
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1986BU14      Nucl.Phys. A457, 337 (1986)

B.L.Burks, R.E.Anderson, T.B.Clegg, E.J.Ludwig, B.C.Karp, Y.Aoki

A DWBA Analysis of the 86Sr(d(pol), p)87Sr Reaction and Implications for a 87Rb Solar Neutrino Detector

NUCLEAR REACTIONS 86Sr(polarized d, p), (polarized d, d), E=11 MeV; measured σ(θ), vector analyzing power versus θ. 87Sr deduced levels, J, π, S. DWBA, optical model analyses.

doi: 10.1016/0375-9474(86)90382-9
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1986KA27      Nucl.Phys. A457, 15 (1986)

B.C.Karp, E.J.Ludwig, J.E.Bowsher, B.L.Burks, T.B.Clegg, F.D.Santos, A.M.Eiro

Alpha-Particle D-State and Configuration-Mixing Effects in the 89Y(d, α)87Sr Reaction

NUCLEAR REACTIONS 89Y(polarized d, α), E=9, 12, 16 MeV; measured σ(θ), vector, tensor analyzing power vs θ. 89Y(polarized d, d), E=12 MeV; measured σ(θ), vector analyzing power vs θ. 87Sr(α, α), E=19.5 MeV; measured σ(θ). 87Sr levels deduced L, J, configuration mixing, α-particle D-state parameter. Finite range DWBA.

doi: 10.1016/0375-9474(86)90517-8
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1985BU14      Nucl.Phys. A442, 300 (1985)

B.L.Burks, R.E.Anderson, T.B.Clegg, E.J.Ludwig, R.L.Varner

Spins and Parities of Low-Lying States in 81Kr from the 80Kr(d(pol), p)81Kr Reaction and Implications for a 81Br Solar Neutrino Detector

NUCLEAR REACTIONS 80Kr(polarized d, p), (polarized d, d), E=11 MeV; 80Kr(polarized p, p), E=16 MeV; measured σ(θ), A(θ). 81Kr levels deduced J, π, S. Enriched gas, ion-implanted foil target. Optical model, DWBA analyses.

doi: 10.1016/0375-9474(85)90147-2
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1985GU09      Nucl.Phys. A438, 187 (1985)

P.P.Guss, R.C.Byrd, C.E.Floyd, C.R.Howell, K.Murphy, G.Tungate, R.S.Pedroni, R.L.Walter, J.P.Delaroche, T.B.Clegg

Cross Sections and Analyzing Powers for Fast-Neutron Scattering to the Ground and First Excited States of 58Ni and 60Ni

NUCLEAR REACTIONS 58,60Ni(n, n), (polarized n, n), (n, n'), E=8-14 MeV; measured σ(θ), analyzing power vs θ; deduced p, n deformation parameters. Optical model, coupled-channels analysis.

doi: 10.1016/0375-9474(85)90124-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12930.


1984DE01      Nucl.Phys. A414, 113 (1984)

J.P.Delaroche, R.L.Varner, T.B.Clegg, R.E.Anderson, B.L.Burks, E.J.Ludwig, J.F.Wilkerson

Structure of Low-Lying States of 76,78,80,82Se Deduced from (p(pol), p') Scattering at 16 MeV

NUCLEAR REACTIONS 76,78,80,82Se(polarized p, p), (polarized p, p'), E=16 MeV; measured σ(θ), A(θ). 76,78,80,82Se deduced deformation parameters. Coupled-channels calculations.

doi: 10.1016/0375-9474(84)90500-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0781.


1984HA22      Nucl.Phys. A419, 45 (1984)

M.Haller, W.Kretschmer, R.E.Anderson, B.L.Burks, T.B.Clegg, E.J.Ludwig, R.L.Varner, J.F.Wilkerson

Investigation of the Reactions 58Ni(d, α)56Co and 50Ti(d, α)48Sc with Vector and Tensor Polarized Deuterons

NUCLEAR REACTIONS 58Ni, 50Ti(d, α), E=16 MeV; measured σ(θ), relative vector, tensor analyzing power vs θ. 56Co, 48Sc levels deduced L-transfer, J, π. DWBA analysis.

doi: 10.1016/0375-9474(84)90284-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1640.


1984WE10      Nucl.Instrum.Methods 219, 284 (1984)

C.R.Westerfeldt, E.G.Bilpuch, M.E.Bleck, D.A.Outlaw, W.K.Wells, J.F.Wilkerson, T.B.Clegg

A System for Producing High-Resolution Polarized and Unpolarized Beams with a Tandem Accelerator

NUCLEAR REACTIONS 54Fe(p, p), E=4.341-4.345 MeV; measured σ(θ) vs E. 55Co deduced resonance, J, π, Γp. R-matrix analysis. 32S(p, p), E=3.374-3.376 MeV; measured T=3/2 resonance yield; deduced optimum resolution conditions. Polarized, unpolarized beams, foil, gas strippers.

doi: 10.1016/0167-5087(84)90334-X
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1983GU03      Nucl.Phys. A395, 1 (1983)

P.P.Guss, K.Murphy, R.C.Byrd, C.E.Floyd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie

The Analyzing Power for the 2H(d, n)3He(g.s.) Reaction from 5.5 to 11.5 MeV

NUCLEAR REACTIONS 2H(polarized d, n), E=5.5, 7, 8.5, 10, 11.5 MeV; measured A(θ). Report discrepancies with previous measurements. Polynomial expansions analysis.

doi: 10.1016/0375-9474(83)90085-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0768.


1983WI04      Nucl.Instrum.Methods 207, 331 (1983)

J.F.Wilkerson, T.B.Clegg, E.J.Ludwig

An Energy Calibration of the TUNL Dual-90° Magnet Analyzing System

NUCLEAR REACTIONS 7Li, 13C, 19F, 27Al, 58Ni(p, n), E ≈ threshold; 12C(p, p), E ≈ 14 MeV; measured yield vs E. Dual 90° magnet system.

doi: 10.1016/0167-5087(83)90644-0
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1983WI15      Phys.Rev.Lett. 51, 2269 (1983)

J.F.Wilkerson, R.E.Anderson, T.B.Clegg, E.J.Ludwig, W.J.Thompson

Isospin and Isobar Components in Light Nuclei

NUCLEAR REACTIONS 28Si(polarized p, p), E=8.011-8.026 MeV; measured σ(θ), A(θ). 29P levels deduced proton isospin-mixing amplitudes. Other data analysis.

doi: 10.1103/PhysRevLett.51.2269
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0066.


1983WO02      Nucl.Phys. A394, 139 (1983)

E.Woye, W.Tornow, G.Mack, C.E.Floyd, P.P.Guss, K.Murphy, R.C.Byrd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie

The Analyzing Power A(y)(θ) for 12C(n, n0, 1)12C between 8.9 and 14.9 MeV Neutron Energy

NUCLEAR REACTIONS 12C(n, n), (n, n'), E=8.9-14.9 MeV; measured A(E, θ); deduced optical potential parameters. 12C level deduced quadrupole deformation.

doi: 10.1016/0375-9474(83)90167-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12993.


1982BU01      Nucl.Phys. A377, 105 (1982)

B.L.Burks, R.R.Cadmus, Jr., T.B.Clegg, E.J.Ludwig

Spins and Parities of Low-Lying States in 79Kr from the 78Kr(d(pol), p)79Kr Reaction

NUCLEAR REACTIONS 78Kr(polarized d, p), (polarized d, d), E=11 MeV; measured σ(θ), A(θ). 79Kr deduced levels, J, π, S. Enriched target. DWBA, optical model analyses.

doi: 10.1016/0375-9474(82)90323-2
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1982BU03      Phys.Rev. C25, 1168 (1982)

B.L.Burks, R.E.Anderson, T.B.Clegg, H.Paetz gen.Schieck, E.J.Ludwig, R.L.Varner, J.F.Wilkerson

Test of the Polarization-Analyzing Power Equality in Two (p(pol), d) Reactions and Their Inverses

NUCLEAR REACTIONS 11B(polarized p, d), E=11.34-11.94 MeV; 13C(polarized p, d), E=13.79-14.39 MeV; measured analyzing power vs E, θ; deduced no definitive time-reversal invariance violation.

doi: 10.1103/PhysRevC.25.1168
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1982FL01      Phys.Rev. C25, 1682 (1982)

C.E.Floyd, P.P.Guss, K.Murphy, C.R.Howell, R.C.Byrd, G.Tungate, S.A.Wender, R.L.Walter, T.B.Clegg

Analyzing Powers for Neutron Elastic Scattering at Forward Angles

NUCLEAR REACTIONS 40Ca, 54Fe, 65Cu, 120Sn, 208Pb(polarized n, n), E=14 MeV; measured A(θ).

doi: 10.1103/PhysRevC.25.1682
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12859.


1982SA12      Phys.Rev. C25, 3243 (1982)

F.D.Santos, S.A.Tonsfeldt, T.B.Clegg, E.J.Ludwig, Y.Tagishi, J.F.Wilkerson

α-Particle D-State Effects in (d, α) Reactions

NUCLEAR REACTIONS 32S, 36,38Ar(polarized d, α), E=16 MeV; analyzed tensor analyzing power data ; deduced α-particle D-state effects. DWBA, Jackson-Riska model D-to S-state ratio.

doi: 10.1103/PhysRevC.25.3243
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1982TA04      Nucl.Phys. A377, 1 (1982)

Y.Tagishi, T.B.Clegg, E.J.Ludwig, S.A.Tonsfeldt, J.F.Wilkerson

Study of (d, α) Reactions on 32S, 36Ar and 38Ar with Vector- and Tensor-Polarized Deuterons

NUCLEAR REACTIONS 32S, 36,38Ar(polarized d, α), E=16 MeV; measured σ(θ), iT11(θ), T20(θ), T22(θ); deduced j-transfer dependence. 30P, 34,36Cl levels deduced L, j-transfer. Enriched targets. DWBA analysis.

doi: 10.1016/0375-9474(82)90318-9
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1982TO11      Nucl.Phys. A385, 373 (1982)

W.Tornow, E.Woye, G.Mack, C.E.Floyd, K.Murphy, P.P.Guss, S.A.Wender, R.C.Byrd, R.L.Walter, T.B.Clegg, H.Leeb

Analyzing Power and Differential Cross Section at 9.9, 11.9 and 13.9 MeV for Ca(n, n)Ca

NUCLEAR REACTIONS 40Ca(polarized n, n), E=9.9, 11.9, 13.9 MeV; measured A(E, θ), σ(E, θ); deduced optical model parameters, Coulomb correction terms. Optical potential analysis, l-dependence, Fourier-Bessel expansion of the real central potential.

doi: 10.1016/0375-9474(82)90093-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12785.


1981FL04      Phys.Rev.Lett. 47, 1042 (1981)

C.E.Floyd, P.P.Guss, K.Murphy, R.C.Byrd, G.Tungate, S.A.Wender, R.L.Walter, T.B.Clegg

Determination of the Spin-Orbit Interaction for Neutron-Nucleus Scattering

NUCLEAR REACTIONS 54Fe, 65Cu(polarized n, n), E=14 MeV; measured σ(θ), A(θ); deduced neutron-nucleus spin-orbit interaction. Optical model.

doi: 10.1103/PhysRevLett.47.1042
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1981LI23      Phys.Rev. C24, 1852 (1981)

P.W.Lisowski, R.C.Byrd, G.Mack, W.Tornow, R.L.Walter, T.B.Clegg, F.D.Santos

Polarization Transfer in (d(pol), n(pol)) Reactions on Light Nuclei at θ = 0°

NUCLEAR REACTIONS 12C, 14N, 16O, 28Si(polarized d, n), E=5-15 MeV; measured polarization transfer. 12C(d, n), E=6-14 MeV; measured σ(θ=0°). DWBA analysis.

doi: 10.1103/PhysRevC.24.1852
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1415.


1981WI03      Nucl.Phys. A362, 8 (1981)

J.E.Willis, T.B.Clegg, M.D.Kaitchuk, E.J.Ludwig, W.J.Thompson

A Polarized Beam Study of the 207Pb(d, t)206Pb Reaction

NUCLEAR REACTIONS 207Pb(polarized d, t), E=15 MeV; measured σ(θ), A(θ). 206Pb levels deduced L, J, π, S. Enriched target, DWBA analysis.

doi: 10.1016/0375-9474(81)90667-9
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1980CL03      Nucl.Phys. A339, 285 (1980)

H.Clement, R.N.Boyd, C.R.Gould, T.B.Clegg

Study of the Structure of the Low-Lying Levels of 29Si via the 28Si(d, pγ) Reaction and Multi-Step Reaction Calculations

NUCLEAR REACTIONS 28Si(polarized d, pγ), E=7.6 MeV; measured pγ(θ). DWBA, CCBA calculations.

doi: 10.1016/0375-9474(80)90094-9
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1980LI03      Nucl.Phys. A334, 45 (1980)

P.W.Lisowski, R.C.Byrd, R.L.Walter, T.B.Clegg

Polarization Transfer of the 2H(p, n)2p Reactions at θ = 0°

NUCLEAR REACTIONS 2H(polarized p, n), E=10.6-15.1 MeV; measured transverse polarization coefficient.

doi: 10.1016/0375-9474(80)90138-4
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1980TH05      Phys.Rev.Lett. 45, 703 (1980)

W.J.Thompson, J.F.Wilkerson, T.B.Clegg, J.M.Feagin, E.J.Ludwig, E.Merzbacher

Atomic-Excitation Effects on Nuclear Reactions

NUCLEAR REACTIONS 12C(polarized p, p), E=14.226-14.236 MeV; measured σ(E, θ), analyzing power vs E, θ. 13N resonance deduced Γ, Γp, atomic excitation effects.

doi: 10.1103/PhysRevLett.45.703
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1177.


1980TO13      Phys.Rev.Lett. 45, 2008 (1980)

S.A.Tonsfeldt, T.B.Clegg, E.J.Ludwig, Y.Tagishi, J.F.Wilkerson

J-Dependent Effects in Tensor Analyzing Powers for the (d, α) Reaction

NUCLEAR REACTIONS 32S, 36,38Ar(polarized d, α), E=16 MeV; measured σ(θ), vector, tensor analyzing power vs θ; deduced angular momentum transfer selectivity of T22. Gas targets.

doi: 10.1103/PhysRevLett.45.2008
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1979CA03      Nucl.Phys. A319, 165 (1979)

R.R.Cadmus, Jr., T.B.Clegg, E.J.Ludwig, S.A.Wender

Spins and Parities of Low-Lying States in 77Kr from the 78Kr(d, t)77Kr Reaction

NUCLEAR REACTIONS 78Kr(polarized d, t), E=15.95 MeV; measured σ(θ), A(θ). 77Kr levels deduced J, π, S. Enriched target. DWBA analysis.

doi: 10.1016/0375-9474(79)90178-7
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1979JE03      Z.Phys. A291, 609 (1979)

M.Jensen, D.R.Tilley, H.R.Weller, N.R.Roberson, S.A.Wender, T.B.Clegg

Polarized-Neutron Capture in the Giant-Resonance Region of 41Ca

NUCLEAR REACTIONS 40Ca(polarized n, γ), E=10 MeV; measured σ(θ), A(θ). 41Ca deduced E2 contribution in giant dipole region. Legendre polynomial analysis.


1979JE05      Phys.Rev.Lett. 43, 609 (1979)

M.Jensen, D.R.Tilley, H.R.Weller, N.R.Robertson, S.A.Wender, T.B.Clegg

Polarized-Neutron Capture In The Giant-Resonance Region Of 41Ca

NUCLEAR REACTIONS 40Ca(n, γ), E=10 MeV; measured products, Eγ, Iγ; deduced σ(θ), polarization data. Data were imported from EXFOR entry 12708.

doi: 10.1103/PhysRevLett.43.609
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1978HE09      Nucl.Phys. A298, 189 (1978)

R.Henneck, T.B.Clegg, R.F.Haglund, Jr., E.J.Ludwig

A Vector-Polarized Beam Study of Fluctuations in 28Si + D Scattering

NUCLEAR REACTIONS 28Si(polarized d, d'), (polarized d, p), E=6-10.46 MeV; measured σ(E, θ), A(E, θ). 30P deduced coherence width, autocorrelations.

doi: 10.1016/0375-9474(78)90251-8
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1978LU03      Phys.Rev.Lett. 40, 441 (1978)

E.J.Ludwig, T.B.Clegg, W.W.Jacobs, S.A.Tonsfeldt

Determination of Angular-Momentum Transfers for (d, α) Reactions Using Polarized Beams

NUCLEAR REACTIONS 28Si, 32S, 40Ca(polarized d, α), E=16.5 MeV; measured A(θ); deduced angular momentum transfer.

doi: 10.1103/PhysRevLett.40.441
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1976IK01      Phys.Rev.Lett. 36, 1357 (1976)

P.G.Ikossi, W.J.Thompson, T.B.Clegg, W.W.Jacobs, E.J.Ludwig

Systematics of Isospin Mixing in Proton Elastic Scattering from Light Nuclei

NUCLEAR REACTIONS 24Mg, 28Si, 32S(p, p); measured σ(E). 8Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca deduced systematics of isospin mixing in elastic p-scattering.

doi: 10.1103/PhysRevLett.36.1357
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1976IK03      Nucl.Phys. A274, 1 (1976); Erratum Nucl.Phys. A279, 532 (1977)

P.G.Ikossi, T.B.Clegg, W.W.Jacobs, E.J.Ludwig, W.J.Thompson

Isospin-Forbidden T=3/2 Resonances in 25Al, 29P and 33Cl, and the Systematics of Isospin Mixing

NUCLEAR REACTIONS 24Mg(p, p), E=5.65-6.25 MeV; 32S(polarized p, p), E=3-3.8 MeV; 28Si(polarized p, p), E=5.6-5.9 MeV; measured σ(E, θ), A(E, θ); deduced optical model parameters. 33Cl, 29P, 25Al, 21Na deduced resonance parameters, reduced widths. Enriched targts, polarized, unpolarized beams.

doi: 10.1016/0375-9474(76)90223-2
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1976LI03      Nucl.Phys. A259, 61 (1976)

P.W.Lisowski, T.C.Rhea, R.L.Walter, C.E.Busch, T.B.Clegg

Scattering of Polarized Neutrons from 3He

NUCLEAR REACTIONS 3He(polarized n, n), E=8.0, 12.0, 17.1 MeV; measured P(θ). 3He(n, n), 1 < E < 23.7 MeV; analyzed, parameterized σ(θ), P(θ), total σ in terms of complex phase shifts.

doi: 10.1016/0375-9474(76)90495-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10590.


1976LI08      Nucl.Phys. A264, 188 (1976)

P.W.Lisowski, R.L.Walter, C.E.Busch, T.B.Clegg

Polarization Transfer Effects in (p, n) Reactions on Light Nuclei at θ = 0°

NUCLEAR REACTIONS 9Be, 11B, 13C(polarized p, n), E=7-15 MeV; measured transverse polarization transfer coefficients.

doi: 10.1016/0375-9474(76)90427-9
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1975LI08      Nucl.Phys. A242, 298 (1975)

P.W.Lisowski, R.L.Walter, C.E.Busch, T.B.Clegg

Polarization Transfer in the 2H(d, n)3He Reaction at θ = 0°

NUCLEAR REACTIONS 2H(d, n), 1 MeV < E < 15 MeV; measured transverse polarization transfer coefficient, tensor analyzing power A.

doi: 10.1016/0375-9474(75)90050-0
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1974BU06      Nucl.Phys. A223, 183 (1974)

C.E.Busch, T.B.Clegg, S.K.Datta, E.J.Ludwig

The Cross Section and Vector Analyzing Power for the Elastic Scattering of 15.0 MeV Deuterons from 10B, 12C, 13C, 14N and 16O

NUCLEAR REACTIONS 10B, 12C, 13C, 14N, 16O(polarized d, d), E=15.0 MeV; measured σ(θ), iT11(θ); deduced optical-model parameters. Natural, enriched targets.

doi: 10.1016/0375-9474(74)90285-1
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1974IK01      Nucl.Phys. A225, 481 (1974)

P.G.Ikossi, C.E.Busch, T.B.Clegg, E.J.Ludwig, W.J.Thompson

A Study of Isobaric Analogue Resonances in 71Ga

NUCLEAR REACTIONS 70Zn(polarized p, p), E=3.6-6.4 MeV; measured σ(E, θ), A(E, θ). 71Ga deduced resonances, J, π, level-width, S.

doi: 10.1016/0375-9474(74)90355-8
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1974LU06      Nucl.Phys. A230, 271 (1974)

E.J.Ludwig, C.E.Busch, T.B.Clegg, S.K.Datta, A.C.Watkins

The Study of (d, t) and (d, 3He) Reactions in Several 1p Shell Nuclei Using Vector-Polarized Beams

NUCLEAR REACTIONS 10B, 14N(polarized d, 3He), 13C, 14N, 10B(polarized d, t), E=15 MeV; measured σ(E(3He), θ), σ(Et, θ), A(θ). 16O(polarized d, t), (polarized d, 3He), E=15 MeV; measured A(θ). 9B, 9Be, 12,13C, 13N levels deduced S, J-dependence, J-admixtures. DWBA analysis. Natural, enriched targets.

doi: 10.1016/0375-9474(74)90307-8
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1974TR02      Nucl.Phys. A220, 533 (1974)

T.A.Trainor, T.B.Clegg, P.W.Lisowski

The Tensor Analyzing Power A(zz) at theta = 0° for the 3He(d, p)4He Reaction

NUCLEAR REACTIONS 3He(polarized d, p), E=6.6-15.8 MeV; measured polarization parameter Azz; θ=0°; enriched target.

doi: 10.1016/0375-9474(74)90133-X
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1974TR06      Phys.Rev.Lett. 33, 229 (1974)

T.A.Trainor, T.B.Clegg, W.J.Thompson

Isospin-Forbidden Proton Partial Width in 41Sc and Similar A = 4n + 1 Nuclei

NUCLEAR REACTIONS 40Ca(polarized p, p), (p, p), E=4975-4981 keV; measured σ(E, θ), A(E, θ). 41Sc deduced J, π, p-width, resonances.

doi: 10.1103/PhysRevLett.33.229
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1974WE01      Phys.Rev.Lett. 32, 177 (1974)

H.R.Weller, N.R.Roberson, D.Rickel, C.P.Cameron, R.D.Ledford, T.B.Clegg

Evidence for E2 and M1 Radiation in the Giant-Dipole-Resonance Region of 15N

NUCLEAR REACTIONS 14C(polarized p, γ), E=4.8-16.2 MeV; measured A(θ), σ(E;Eγ, θ). 15N resonances deduced J, π, γ-multipolarities.

doi: 10.1103/PhysRevLett.32.177
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1973CL05      Phys.Rev. C8, 922 (1973)

T.B.Clegg, D.D.Armstrong, R.A.Hardekopf, P.W.Keaton, Jr.

Polarization Transfer in the 2H(d, p)3H Reaction at theta = 0°

NUCLEAR REACTIONS 2H(polarized d, p), E=6-15 MeV, θ=0°; measured polarization transfer(E).

doi: 10.1103/PhysRevC.8.922
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1973DA26      Phys.Rev.Lett. 31, 949 (1973)

S.K.Datta, C.E.Busch, T.B.Clegg, E.J.Ludwig, W.J.Thompson

Comparison of Vector Analyzing Powers in (d, d) with Those (d, 3He) and (d, t) l = 0 Transfer Reactions

NUCLEAR REACTIONS 14N, 30Si(polarized d, t), (polarized d, d), 32S(polarized d, d), (polarized d, 3He), E=15 MeV; measured analyzing power A(θ).

doi: 10.1103/PhysRevLett.31.949
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1973GO02      Phys.Rev.Lett. 30, 298 (1973)

C.R.Gould, R.O.Nelson, J.R.Williams, D.R.Tilley, J.D.Hutton, N.R.Robertson, C.E.Busch, T.B.Clegg

Application of Polarized Deuterons in (d, pγ) Angular Correlation Measurements

NUCLEAR REACTIONS 12C, 30Si(d, pγ), E=4.15 MeV; measured pγ(θ). 13C, 31Si transitions deduced γ-mixing.

doi: 10.1103/PhysRevLett.30.298
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1973IK04      Bull.Am.Phys.Soc. 18, 254, BB10 (1973), See Keyno. 1973IKZY

P.G.Ikossi, C.E.Busch, T.B.Clegg, E.J.Ludwig, W.J.Thompson

Cross Sections and Polarizations for Isobaric Analog Resonances in 71Ga


1973LU04      Nucl.Phys. A211, 559 (1973)

E.J.Ludwig, T.B.Clegg, R.L.Walter

The Polarization of 3He Elastically Scattered from 27Al and 28Si at 21 MeV

NUCLEAR REACTIONS 27Al, 28Si(3He, 3He); E=21 MeV; measured σ(θ), P(θ). Deduced optical-model parameters. Natural targets.

doi: 10.1016/0375-9474(73)90443-0
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1973VO02      Nucl.Phys. A204, 529 (1973); Erratum Nucl.Phys. A217, 628 (1973)

H.J.Votava, T.B.Clegg, E.J.Ludwig, W.J.Thompson

Proton Scattering from 9Be between 6 and 30 MeV and the Structure of 9Be

NUCLEAR REACTIONS 9Be(p, p0), (p, p2); measured σ(θ), E=13.0, 14.0, 15.0, 21.35, 30.3 MeV; measured vector polarization analyzing power A(θ), E=8.0, 11.0, 12.0, 13.0, 15.0 MeV; measured σ(E, θ), θ(lab)=86.9°, 120°, 140°, 160°, 6 < E < 15 MeV. 9Be(p, d0)8Be; measured σ(θ), E=13.0, 14.0, 15.0, 21.35, 30.3 MeV; measured A(θ), E=8.0, 11.0, 12.0, 13.0, 15.0 MeV. Natural target. 9Be deduced deformation parameter.

doi: 10.1016/0375-9474(73)90393-X
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1972HA14      Phys.Rev.Lett. 28, 760 (1972)

R.A.Hardekopf, R.L.Walter, T.B.Clegg

Polarization Differences in the Reactions D(d, t)T and D(d, n)3He and Charge Symmetry

NUCLEAR REACTIONS 3H(polarized p, d), E=2-14 MeV; measured polarization P(E;θ); compared 2H(d, p), 2H(d, n) polarizations.

doi: 10.1103/PhysRevLett.28.760
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1972HA51      Nucl.Phys. A191, 481 (1972)

R.A.Hardekopf, P.W.Lisowski, T.C.Rhea, R.L.Walter, T.B.Clegg

Four-Nucleon Studies (IV). Analyzing Powers in the Elastic Scattering Of Protons from Tritium

NUCLEAR REACTIONS 3H(polarized p, p)3H, Ep=6.7, 7.4, 8.0, 9.4, 10.7, 12.0, 13.4, 14.7 MeV; measured P(θ).

doi: 10.1016/0375-9474(72)90626-4
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1972MC01      Nucl.Phys. A178, 529 (1972)

W.S.McEver, T.B.Clegg, J.M.Joyce, E.J.Ludwig

The Polarization of 3He Particles Elastically Scattered from 9Be, 12C and 16O

NUCLEAR REACTIONS 9Be, 12C, 16O(3He, 3He), E=18 MeV; measured P(θ); deduced optical model parameters.

doi: 10.1016/0375-9474(72)90479-4
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1971SC04      Nucl.Phys. A163, 432 (1971)

P.Schwandt, T.B.Clegg, W.Haeberli

Polarization Measurements and Phase Shifts for p-4He Scattering between 3 and 18 MeV

NUCLEAR REACTIONS 4He(polarized p, p), E=4.58, 5.95, 7.89, 9.89, 11.94 MeV; measured polarization P(E, θ); deduced scattering phase shifts. Natural target.

doi: 10.1016/0375-9474(71)90500-8
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1970MC07      Phys.Lett. 31B, 560 (1970)

W.S.McEver, T.B.Clegg, J.M.Joyce, E.J.Ludwig, R.L.Walter

An Analyzer for the Polarization of 3He Particles

NUCLEAR REACTIONS 4He(polarized 3He, 3He), E=11.5-13 MeV; measured analyzing power(E(3He)).

doi: 10.1016/0370-2693(70)90692-1
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1970MC10      Phys.Rev.Lett. 24, 1123 (1970)

W.S.McEver, T.B.Clegg, J.M.Joyce, E.J.Ludwig, R.L.Walter

Polarization of 3He Scattered from 12C

NUCLEAR REACTIONS 12C(3He, 3He), E=18, 20 MeV; measured P(θ), σ(θ); deduced optical model parameters.

doi: 10.1103/PhysRevLett.24.1123
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1969KO08      Nucl.Phys. A132, 455 (1969)

D.C.Kocher, T.B.Clegg

Cross Sections for Proton-Deuteron Scattering from 1.0 to 10.0 MeV

NUCLEAR REACTIONS 2H(p, p); E=1-10 MeV; measured σ(θ, E). Enriched target.

doi: 10.1016/0375-9474(69)90496-5
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1969MC02      Nucl.Phys. A126, 233(1969)

D.H.McSherry, S.D.Baker, G.R.Plattner, T.B.Clegg

Measurement of Spin-Correlation Effects in p-3He Elastic Scattering at 8.8 MeV

NUCLEAR REACTIONS 3He(polarized p, p); aligned nuclide; E=8.8 MeV; measured spin-correlation parameter A(xz); deduced phase shifts. Enriched target.

doi: 10.1016/0375-9474(69)90410-2
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1968CL07      Nucl.Phys. A119, 238(1968)

T.B.Clegg, G.R.Plattner, W.Haeberli

Polarization of Protons Elastically Scattered from Deuterons at 12.0 MeV

NUCLEAR REACTIONS 2H(p, p), E=12 MeV; measured polarization (θ). Enriched target.

doi: 10.1016/0375-9474(68)90818-X
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1968PL01      Nucl.Phys. A111, 481(1968)

G.R.Plattner, T.B.Clegg, L.G.Keller

The Analysing Power of the Reaction 7Li(p, α)4He for Polarized Protons From 3 to 10 MeV

NUCLEAR REACTIONS 7Li(p, α), E=3-10 MeV; measured polarization analyzing power (E, θ). Enriched target.

doi: 10.1016/0375-9474(68)90234-0
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1967CL04      Nucl.Phys. A95, 608(1967)

T.B.Clegg, W.Haeberli

Polarization of Protons Elastically Scattered from Deuterons from 4 to 12 MeV

NUCLEAR REACTIONS 2H(p, p), 2H(p, pn), 12C(p, p), 12C(p, p'), E = 4-12 MeV; measured polarization (E, θ). Enriched 2H target, natural C target.

doi: 10.1016/0375-9474(67)90853-6
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1967TR09      Phys.Letters 25B, 585 (1967)

W.Trachslin, L.Brown, T.B.Clegg, R.G.Seyler

Polarization and Phase Shifts in D(p, p)d at 3.00 MeV

NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90122-0
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1966BA35      Nucl.Phys. 86, 130(1966)

A.C.L.Barnard, J.B.Swint, T.B.Clegg

Cross Sections as a Function of Angle and Complex Phase Shifts for the Scattering of Protons from 12C

NUCLEAR REACTIONS 12C(p, p), E = 2.4-11.6 MeV; 12C(p, p'), E = 6.6-11.6 MeV; 12C(p, α), E = 11.6 MeV; measured σ(E;θ). Natural target.

doi: 10.1016/0029-5582(66)90296-3
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1966SW04      Nucl.Phys. 86, 119(1966)

J.B.Swint, A.C.L.Barnard, T.B.Clegg, J.L.Weil

Cross Sections as a Function of Energy for the Scattering of Protons from 12C

NUCLEAR REACTIONS 12C(p, p), E = 4.7-12.8 MeV; 12C(p, p'), E = 6.0-12.8 MeV; measured σ(E, θ). 13N deduced levels. Natural target.

doi: 10.1016/0029-5582(66)90295-1
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1965SW01      Bull.Am.Phys.Soc. 10, No.2, 155, A7 (1965)

J.B.Swint, A.C.L.Barnard, T.B.Clegg

Scattering of Protons by 12C

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.


1964CL03      Nucl. Phys. 50, 621 (1964)

T.B.Clegg, A.C.L.Barnard, J.B.Swint, J.L.Weil

The Elastic Scattering of Protons from He3 from 4.5 to 11.5 MeV

doi: 10.1016/0029-5582(64)90234-2
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1964SW02      Bull.Am.Phys.Soc. 9, No.4, 408, CA11 (1964)

J.B.Swint, T.B.Clegg, J.L.Weil, C.M.Jones, A.C.L.Barnard

Scattering of Protons by 12C

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.


1963CL01      Bull.Am.Phys.Soc. 8, No.2, 124, U3 (1963)

T.B.Clegg, A.C.L.Barnard, J.B.Swint, J.L.Weil

He3(p, p)He3, 4.5-10.4 MeV

NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.


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