NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = T.B.Clegg Found 85 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1969KO08 Nucl.Phys. A132, 455 (1969) 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
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
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
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
1967CL04 Nucl.Phys. A95, 608(1967) 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
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
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
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
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
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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