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NSR database version of April 11, 2024.

Search: Author = E.J.Ludwig

Found 87 matches.

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2006FI06      Phys.Rev. C 74, 034001 (2006)

B.M.Fisher, C.R.Brune, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, T.C.Black, M.Viviani, A.Kievsky, S.Rosati

Proton-3He elastic scattering at low energies

NUCLEAR REACTIONS 3He(p, p), (polarized p, p), E=0.99, 1.59, 2.24, 3.11, 4.02 MeV; measured σ(θ), Ay(θ). Four-body variational calculations with realistic two- and three-body interactions.

doi: 10.1103/PhysRevC.74.034001
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1467.


2006LE19      Phys.Rev. C 73, 045801 (2006)

D.S.Leonard, H.J.Karwowski, C.R.Brune, B.M.Fisher, E.J.Ludwig

Precision measurements of 2H(d, p)3H and 2H(d, n)3He total cross sections at Big Bang nucleosynthesis energies

NUCLEAR REACTIONS 2H(d, p), (d, n), E=120-650 keV; measured Ep, En, σ(E, θ); deduced integrated σ. Astrophysical implications discussed.

doi: 10.1103/PhysRevC.73.045801
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1499.


2004BR08      Phys.Rev. C 69, 024608 (2004)

B.Braizinha, C.R.Brune, A.M.Eiro, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, F.D.Santos, I.J.Thompson

Resonant and direct components in the 3He(d, p)4He reaction at low energies

NUCLEAR REACTIONS 3He(polarized d, p), E=0.52, 0.89, 1.49 MeV; measured σ(θ=0°), analyzing power; deduced scattering matrix elements.

doi: 10.1103/PhysRevC.69.024608
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0978.


2003KE05      Phys.Rev. C 67, 044604 (2003)

N.Keeley, T.L.Drummer, E.E.Bartosz, C.R.Brune, P.D.Cathers, M.Fauerbach, H.J.Karwowski, K.W.Kemper, B.Kozlowska, E.J.Ludwig, F.Marechal, A.J.Mendez, E.G.Myers, D.Robson, K.Rusek, K.D.Veal

Multistep processes in the 12C(6Li, d) stripping reaction

NUCLEAR REACTIONS 12C(polarized 6Li, d), E=34, 50 MeV; measured σ(E, θ), analyzing powers; deduced multistep transfer contributions. Coupled reaction channels calculations.

doi: 10.1103/PhysRevC.67.044604
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0983.


2002FL03      Phys.Rev. C 66, 057601 (2002)

K.A.Fletcher, C.R.Brune, B.M.Fisher, R.P.Fitzgerald, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, R.C.Runkle, M.H.Wood, W.H.Geist, K.D.Veal, G.M.Hale

Kyy'(O°) for 3He(d, p)4He near the Jπ=3/2+ resonance

NUCLEAR REACTIONS 3He(polarized d, p), E=520, 890, 1490 keV; measured polarization transfer coefficient. 5Li deduced resonance.

doi: 10.1103/PhysRevC.66.057601
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0943.


2002WO05      Phys.Rev. C65, 034002 (2002)

M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, A.Kievsky, S.Rosati, M.Viviani

Low-Energy p-d Scattering: High-Precision data, comparisons with theory, and phase-shift analyses

NUCLEAR REACTIONS 2H(polarized p, p), 1H(polarized d, d), E(cm)=667 keV; measured σ(θ), Ay(θ), other analyzing powers; deduced phase shift parameters. Comparison with NN and 3N model predictions.

doi: 10.1103/PhysRevC.65.034002
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0891.


2001BR12      Phys.Rev. C63, 044013 (2001)

C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal, M.H.Wood, A.Kievsky, S.Rosati, M.Viviani

Proton-Deuteron Elastic Scattering at Low Energies

NUCLEAR REACTIONS 2H(polarized p, p), E=431.3-2000 keV; measured σ(θ), analyzing power vector and tensor components. Comparison with calculations using hyperspherical harmonic basis and different nuclear potentials.

doi: 10.1103/PhysRevC.63.044013
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0801.


2001KI03      Phys.Rev. C63, 024005 (2001)

A.Kievsky, M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, S.Rosati, M.Viviani

Evidence for Three Nucleon Force Effects in p-d Elastic Scattering

NUCLEAR REACTIONS 2H(p, p), E=1 MeV; measured σ(θ); deduced contribution from three-nucleon force. Comparisons with model predictions.

doi: 10.1103/PhysRevC.63.024005
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0891.


2001KI22      Nucl.Phys. A689, 349c (2001)

A.Kievsky, M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, S.Rosati, M.Viviani

χ2 Analysis of p-d Differential Cross Sections at Low Energies

NUCLEAR REACTIONS 1H(d, d), E=1 MeV; measured σ(θ); deduced model parameters.

doi: 10.1016/S0375-9474(01)00852-1
Citations: PlumX Metrics


2001WO06      Nucl.Phys. A684, 549c (2001)

M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, A.Kievsky, D.S.Leonard, E.J.Ludwig, S.Rosati, M.Viviani

Low Energy P-D Elastic Scattering and the ' Ay Puzzle '

NUCLEAR REACTIONS 2H(polarized p, p), E(cm)=667 keV; measured σ(θ), Ay(θ), tensor analyzing powers. Comparisons with model predictions.

doi: 10.1016/S0375-9474(01)00390-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1236.


2000CR01      Phys.Rev. C61, 034006 (2000)

B.J.Crowe III, C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal, A.C.Fonseca, G.M.Hale, K.A.Fletcher

Analyzing Powers for 2H(d(pol), d)2H at Deuteron Energies of 3.0, 4.75, and 6.0 MeV

NUCLEAR REACTIONS 2H(polarized d, d), E=3.0, 4.75, 6.0 MeV; measured tensor analyzing powers vs θ; deduced nucleon-nucleon p-wave contributions. R matrix parameterization, microscopic four-body calculations.

doi: 10.1103/PhysRevC.61.034006
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0649.


2000FL08      Nucl.Instrum.Methods Phys.Res. A455, 620 (2000)

K.A.Fletcher, W.H.Geist, C.R.Brune, B.M.Fisher, R.P.Fitzgerald, H.J.Karwowski, D.E.Kruse, D.S.Leonard, E.J.Ludwig, R.C.Runkle, K.D.Veal, M.H.Wood

A Proton Polarimeter for 3He(d, p)4He Polarization Transfer Studies

NUCLEAR REACTIONS 3He(d, p), E=430 keV; measured proton polarization, effective analyzing power vs Ep. Comparison with Monte Carlo simulation.

doi: 10.1016/S0168-9002(00)00569-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1348.


1999BL26      Phys.Lett. 471B, 103 (1999)

T.C.Black, H.J.Karwowski, E.J.Ludwig, A.Kievsky, S.Rosati, M.Viviani

Determination of Proton-Deuteron Scattering Lengths

NUCLEAR REACTIONS 2H(p, p), E(cm)=0.163-2 MeV; calculated σ(θ), doublet and quartet S-wave effective range function, phase shifts; deduced singularity in doublet S-wave effective range function. Three nucleon interaction.

doi: 10.1016/S0370-2693(99)01366-0
Citations: PlumX Metrics


1999GE19      Phys.Rev. C60, 054003 (1999); Erratum Phys.Rev. C67, 059904 (2003)

W.H.Geist, C.R.Brune, H.J.Karwowski, E.J.Ludwig, K.D.Veal, G.M.Hale

The 3He(d(pol), p)4He Reaction at Low Energies

NUCLEAR REACTIONS 3H(polarized d, p), E=60-641 keV; measured σ(E, θ), Ay(E, θ), Azz(E, θ), Ayy(E, θ), Axz(E, θ); deduced low-energy S-factor, electron screening potential. 5Li deduced levels, J, π. R-matrix analysis.

doi: 10.1103/PhysRevC.60.054003
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0594.


1999KA46      Acta Phys.Pol. B30, 1479 (1999)

H.J.Karwowski, C.R.Brune, W.H.Geist, E.J.Ludwig, K.D.Veal, M.H.Wood, A.Kievsky, S.Rosati, M.Viviani, T.C.Black

New Physics in p-d Elastic Scattering at Low Energies

NUCLEAR REACTIONS 2H(polarized p, p), E(cm)=0.163-2 MeV; 1H(polarized d, d), E(cm)=0.163-2 MeV; measured σ, vector and tensor analyzing powers; deduced NN potential features, role of 3-body force. Pair-Correlated Hyperspherical Harmonic Calculations.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0801.


1999VE11      Phys.Rev. C60, 064003 (1999)

K.D.Veal, C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, E.E.Bartosz, P.D.Cathers, T.L.Drummer, K.W.Kemper, A.M.Eiro, F.D.Santos, B.Kozlowska, H.J.Maier, I.J.Thompson

Determination of the Asymptotic D- to S-State Ratio for 6Li via (6Li(pol), d) Transfer Reactions

NUCLEAR REACTIONS 40Ca, 58Ni(polarized 6Li, d), E=34 MeV; measured deuteron spectra, σ(E, θ), Ay(θ), tensor analyzing powers. 6Li deduced asymptotic D- to S-state ratio. DWBA analysis.

doi: 10.1103/PhysRevC.60.064003
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0607.


1998BL05      Nucl.Phys. A631, 680c (1998)

T.-C.Black, H.-J.Karwowski, E.-J.Ludwig, A.Kievsky, S.Rosati, M.Viviani

An Energy-Dependent Phase Shift Analysis of Low-Energy Proton-Deuteron Elastic Scattering

doi: 10.1016/S0375-9474(98)00090-6
Citations: PlumX Metrics


1998BR10      Phys.Rev. C57, 3437 (1998)

C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal

9Be(p(pol), d)8Be and 9Be(p(pol), α)6Li Reactions at Low Energies

NUCLEAR REACTIONS 9Be(polarized p, d), (polarized p, α), E=77-321 keV; measured σ(θ), A(y)(θ); deduced reaction mechanism. R-matrix, DWBA analyses. Implications for stellar reaction rates discussed.

doi: 10.1103/PhysRevC.57.3437
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0552.


1998BR11      Phys.Lett. 428B, 13 (1998)

C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal, M.H.Wood, A.Kievsky, S.Rosati, M.Viviani

Possible Three-Nucleon Force Effects in D-P Scattering at Low Energies

NUCLEAR REACTIONS 2H(polarized p, p), E(cm)=432 keV; measured A(y)(θ), iT11(θ); deduced possible three-nucleon force effects.

doi: 10.1016/S0370-2693(98)00370-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0801.


1998VE03      Phys.Rev.Lett. 81, 1187 (1998)

K.D.Veal, C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, A.J.Mendez, E.E.Bartosz, P.D.Cathers, T.L.Drummer, K.W.Kemper, A.M.Eiro, F.D.Santos, B.Kozlowska, H.J.Maier, I.J.Thompson

Deformation Effects in 6Li

NUCLEAR REACTIONS 58Ni(polarized 6Li, d), E=34 MeV; analyzed σ(θ), A(y)(θ), A(zz)(θ), A(xz)(θ). 6Li deduced asymptototic D- to S-state ratio. DWBA analysis.

doi: 10.1103/PhysRevLett.81.1187
Citations: PlumX Metrics


1997BR37      Nucl.Instrum.Methods Phys.Res. A389, 421 (1997)

C.R.Brune, H.J.Karwowski, E.J.Ludwig

Determination of Low-Energy Proton Polarization Via the 6Li(p(pol), 3He)4He Reaction

NUCLEAR REACTIONS 6Li(polarized p, 3He), E=250-460 MeV; measured A(y)(θ). 4He(polarized p, p), E=6 MeV; measured A(y); deduced beam polarization.

doi: 10.1016/S0168-9002(97)00340-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0491.


1997KI17      Phys.Lett. 406B, 292 (1997)

A.Kievsky, S.Rosati, M.Viviani, C.R.Brune, H.J.Karwowski, E.J.Ludwig, M.H.Wood

The Three-Nucleon System Near the N-d Threshold

NUCLEAR REACTIONS 1H(polarized d, d), E(cm)=432 keV; measured tensor analyzing powers vs θ; deduced scattering wave functions, three-nucleon properties.

doi: 10.1016/S0370-2693(97)00691-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0801.


1997MA08      Phys.Rev. C55, 588 (1997)

L.Ma, H.J.Karwowski, C.R.Brune, Z.Ayer, T.C.Black, J.C.Blackmon, E.J.Ludwig, M.Viviani, A.Kievsky, R.Schiavilla

Measurements of 1H(d(pol), γ)3He and 2H(p(pol), γ)3He at Very Low Energies

NUCLEAR REACTIONS 1H(polarized d, γ), E(cm)=40-110 keV; 2H(polarized p, γ), E(cm)=70-210 keV; measured σ(θ), analyzing powers vs θ; deduced thermonuclear reaction rate.

doi: 10.1103/PhysRevC.55.588
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0539.


1996GE15      Nucl.Instrum.Methods Phys.Res. B111, 176 (1996)

W.H.Geist, Z.Ayer, A.C.Hird, E.J.Ludwig, M.Wood, K.A.Fletcher

Ion Implanted 3He Targets for Very Low Energy Experiments

NUCLEAR REACTIONS 3He(polarized d, p), E=322 keV; measured A(yy)(θ); deduced target characteristics. 3He ions implanted in tantalum, aluminum.

doi: 10.1016/0168-583X(95)01268-0
Citations: PlumX Metrics


1995AY03      Phys.Rev. C52, 2851 (1995)

Z.Ayer, H.J.Karwowski, B.Kozlowska, E.J.Ludwig

Determination of the Asymptotic D- to S-State Ratio for 3He via (d(pol), 3He) Reactions

NUCLEAR REACTIONS 93Nb(polarized d, 3He), E=12 MeV; 63Cu(polarized d, 3He), E=8 MeV; 89Y(polarized d, 3He), E=10.5 MeV; 93Nb(polarized d, d), E=12 MeV; measured σ(θ), tensor analyzing powers vs θ. 3He deduced D-state parameter. Finite-range DWBA analysis. Enriched targets.

doi: 10.1103/PhysRevC.52.2851
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0429.


1995GE16      Nucl.Instrum.Methods Phys.Res. A365, 36 (1995)

W.Geist, Z.Ayer, A.C.Hird, H.J.Karwowski, E.J.Ludwig

A Deuteron Tensor Polarimeter for Low-Energy Experiments

NUCLEAR REACTIONS 3He(polarized d, p), E=121-311 keV; measured tensor analyzing power vs θ; deduced polarimeter calibration.

doi: 10.1016/0168-9002(95)00456-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1429.


1994FL03      Phys.Rev. C49, 2305 (1994)

K.A.Fletcher, Z.Ayer, T.C.Black, R.K.Das, H.J.Karwowski, E.J.Ludwig, G.M.Hale

Tensor Analyzing Power for 2H(d, p)3H and 2H(d, n)3He at Deuteron Energies of 25, 40, 60, and 80 keV

NUCLEAR REACTIONS 2H(polarized d, p), (polarized d, n), E=25-80 keV; measured σ(θ), tensor analyzing power vs θ; deduced implications for neutron-lean fusion reaction, entrance channel quintent S-state role.

doi: 10.1103/PhysRevC.49.2305
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0138.


1994KO29      Phys.Rev. C50, 2695 (1994)

B.Kozlowska, Z.Ayer, R.K.Das, H.J.Karwowski, E.J.Ludwig

Determination of the Asymptotic D- to S-State Ratio of the Triton from Sub-Coulomb (d(pol), t) Reactions

NUCLEAR REACTIONS 119Sn(polarized d, t), E=5.25 MeV; 149Sm(polarized d, t), E=6 MeV; 206Pb(polarized d, t), E=10 MeV; measured tensor analyzing power vs θ. 3H deduced asymptotic D- to S-state ratio. Finite-range DWBA analysis.

doi: 10.1103/PhysRevC.50.2695
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0566.


1993CR01      Phys.Rev. C47, 2690 (1993)

E.R.Crosson, S.K.Lemieux, E.J.Ludwig, W.J.Thompson, M.Bisenberger, R.Hertenberger, D.Hofer, H.Kader, P.Schiemenz, G.Graw, A.M.Eiro, F.D.Santos

Probing α-Particle Wave Functions Using (d(pol), α) Reactions

NUCLEAR REACTIONS 50Ti, 58Ni(polarized d, α), E=16, 22 MeV; measured σ(θ), vector, tensor analyzing power vs θ; deduced α-particle D-state role. Exact finite-range DWBA analysis.

doi: 10.1103/PhysRevC.47.2690
Citations: PlumX Metrics


1993CR04      Phys.Rev. C48, 1770 (1993)

E.R.Crosson, E.J.Ludwig, M.Bisenberger, R.Hertenberger, D.Hofer, H.Kader, P.Schiemenz, G.Graw, A.M.Eiro, F.D.Santos, B.A.Brown

Configuration Mixing in 56Co and 46Sc Using (d(pol), α) Reactions

NUCLEAR REACTIONS 58Ni, 48Ti(polarized d, α), E=22 MeV; measured σ(θ), analyzing power vs θ. 56Co, 46Sc levels deduced L-mixing ratios.

doi: 10.1103/PhysRevC.48.1770
Citations: PlumX Metrics


1993FL06      Nucl.Instrum.Methods Phys.Res. A329, 197 (1993)

K.A.Fletcher, T.C.Black, H.J.Karwowski, E.J.Ludwig, Y.Tagishi

A Deuteron Tensor Polarimeter for Energies Below 90 keV

NUCLEAR REACTIONS 2H(polarized d, p), E=20-90 keV; measured analyzing power at θ=10°; deduced deuteron tensor polarimeter characteristics.

doi: 10.1016/0168-9002(93)90936-C
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1416.


1992CR01      Phys.Rev. C45, R492 (1992)

E.R.Crosson, R.K.Das, S.K.Lemieux, E.J.Ludwig, W.J.Thompson, M.Bisenberger, R.Hertenberger, D.Hofer, H.Kader, P.Schiemenz, G.Graw, A.M.Eiro, F.D.Santos

Probing α-Particle Wave Functions by (d, α) Tensor Analyzing Powers

NUCLEAR REACTIONS 58Ni(polarized d, α), E=22 MeV; 50Ti(polarized d, α), E=16 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 4He deduced D-state parameters. DWBA analysis, realistic interactions.

doi: 10.1103/PhysRevC.45.R492
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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


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
Citations: PlumX Metrics


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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1986BH07      Phys.Rev. C34, 736 (1986)

C.M.Bhat, Y.Tagishi, E.J.Ludwig, B.A.Brown

36,38Ar(d(pol), α)34,36Cl Reactions Induced by Tensor Polarized Deuterons

NUCLEAR REACTIONS 36,38Ar(polarized d, α), E=16 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ. 34,36Cl levels deduced two-nucleon spectroscopic amplitudes. Shell model.

doi: 10.1103/PhysRevC.34.736
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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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1986BU18      Phys.Rev. C34, 2316 (1986)

B.L.Burks, R.L.Varner, E.J.Ludwig

Q-Value Determination for the 80Kr(d, p)81Kr Reaction

NUCLEAR REACTIONS 80Kr(d, p), E=11 MeV; measured σ(Ep); deduced Q. 80Kr deduced mass excess. Ion implanted foil target.

doi: 10.1103/PhysRevC.34.2316
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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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1985SA18      Phys.Rev. C32, 338 (1985)

F.D.Santos, B.C.Karp, J.E.Bowsher, E.J.Ludwig, A.M.Eiro

Determination of Two-Nucleon Spectroscopic Amplitudes from (d, α) Analyzing Powers

NUCLEAR REACTIONS 89Y(d, α), E=9, 12, 16 MeV; measured σ(θ), vector, tensor analyzing power vs θ. 87Sr levels deduced L, J, mixing amplitudes. Finite-range DWBA, S-, D-state admixture, neutron, proton configurations involved.

doi: 10.1103/PhysRevC.32.338
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1984BU23      Phys.Rev. C30, 742 (1984)

B.L.Burks, R.E.Anderson, Y.Aoki, B.C.Karp, E.J.Ludwig, W.J.Thompson, R.L.Varner

81Kr-81Br Ground-State Mass Difference and Implications for Calibration of a 81Br Solar Neutrino Detector

NUCLEAR REACTIONS 82Kr(d, t), (d, 3He), E=17 MeV; measured σ(Et), σ(E(3He)); deduced Q-value difference. 81Kr, 81Br deduced mass difference.

doi: 10.1103/PhysRevC.30.742
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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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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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1984KA33      Phys.Rev.Lett. 53, 1619 (1984)

B.C.Karp, E.J.Ludwig, W.J.Thompson, F.D.Santos

α-Particle D-State Components from (d, α) Analyzing Powers

NUCLEAR REACTIONS 89Y(polarized d, α), E=9, 12, 16 MeV; measured σ(θ), analyzing power vs θ. 4He deduced D-state parameter. Exact finite-range DWBA analysis.

doi: 10.1103/PhysRevLett.53.1619
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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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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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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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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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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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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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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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1977BA14      Nucl.Phys. A278, 217 (1977)

A.K.Basak, J.A.R.Griffith, M.Irshad, O.Karban, E.J.Ludwig, J.M.Nelson, S.Roman, G.Tungate

Spectroscopy of the 50Cr(d, p)51Cr Reaction and the Deuteron d-State Effects

NUCLEAR REACTIONS 50Cr(polarized d, p), E=12.3 MeV; measured analyzing powers iT11(θ), T20(θ), T22(θ). 51Cr levels deduced J. Enriched target.

doi: 10.1016/0375-9474(77)90236-6
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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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1974BA49      Nucl.Phys. A229, 219 (1974)

A.K.Basak, J.A.R.Griffith, M.Irshad, O.Karban, E.J.Ludwig, J.M.Nelson, S.Roman

Vector Analyzing Power of (d, p) and (d, t) Reactions on 142Nd at 12.3 MeV

NUCLEAR REACTIONS 142Nd(polarized d, d), (polarized d, p), (polarized d, t), E=12.3 MeV; measured iT11(θ); deduced optical-model parameters, reaction characteristics. 143Nd levels deduced L(n), J, S; 141Nd levels deduced L(n), J. Enriched target.

doi: 10.1016/0375-9474(74)90784-2
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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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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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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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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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1971LU13      Part.Nucl.2, 107 (1971)

E.J.Ludwig, W.J.Thompson, H.J.Votava

Nuclear Scattering Potentials for Composite Projectiles


1970DZ04      Phys.Lett. 33B, 302 (1970)

T.G.Dzubay, A.A.Jaffe, E.J.Ludwig, T.A.White, F.Everling, D.W.Miller, D.A.Outlaw

Energy Levels of 36K

NUCLEAR REACTIONS 36Ar(3He, t), E=22.17 MeV; measured σ(Et), Q. 36K deduced levels, mass excess.

doi: 10.1016/0370-2693(70)90276-5
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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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1970MC12      Nucl.Phys. A147, 81 (1970)

J.E.McQueen, Jr., J.M.Joyce, E.J.Ludwig

The 30Si(3He, α)29Si Reaction at 8.0 and 7.0 MeV

NUCLEAR REACTIONS 30Si(3He, 3He), E = 8.0, 7.0 MeV; measured σ(θ). 30Si(3He, α), E = 6.8 to 8.2 MeV; measured σ(E;Eα, θ). 29Si levels deduced L, S. Enriched target.

doi: 10.1016/0375-9474(70)90511-7
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1970MC18      Nucl.Phys. A151, 295 (1970)

J.E.McQueen, Jr., J.M.Joyce, E.J.Ludwig

The (3He, α) Reaction with Nuclei in the s-d Shell

NUCLEAR REACTIONS 24,26Mg, 28Si, 32S(3He, 3He), (3He, α), E=8 MeV; measured σ(θ), σ(Eα, θ); deduced optical model parameters. 24Mg, 28Si(3He, α), E=6.8-8.2 MeV; measured σ(E, Eα, θ). 23,25Mg, 27Si, 31S levels deduced L, S. Enriched targets.

doi: 10.1016/0375-9474(70)90281-2
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1969FI04      Nucl.Phys. A131, 267 (1969)

S.Fiarman, E.J.Ludwig, L.S.Michelman, A.B.Robbins

Proton Polarization Measurements Near Isobaric Analogue Resonances in 145Eu

NUCLEAR REACTIONS 144Sm(p, p), E=9.1-11.2 MeV; measured polarization P(E;θ). 145Eu resonances deduced J.

doi: 10.1016/0375-9474(69)90536-3
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1969MI09      Phys.Rev. 180, 1114 (1969)

L.S.Michelman, S.Fiarman, E.J.Ludwig, A.B.Robbins

Study of the 90Zr(d, p)91Zr Reaction

NUCLEAR REACTIONS 90Zr(d, p), (d, d), E=11 MeV; 91Zr(p, p), E=14.8, 16 MeV; measured σ(θ), P(θ); deduced optical model parameters.

doi: 10.1103/PhysRev.180.1114
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1966FI03      Phys.Letters 22, 175 (1966)

S.M.Fiarman, E.J.Ludwig, L.Michelman, A.B.Robbins

Isobaric Analogue State Polarization Measurements to Determine the Spin of 145Sm

NUCLEAR STRUCTURE 145Sm, 145Eu; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90564-6
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1965LU03      Phys.Rev. 138, B364 (1965)

E.J.Ludwig, D.W.Miller

Proton Polarization in the Sr88(d, p)Sr89* (1.05-Mev) Reaction

NUCLEAR STRUCTURE 89Sr; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.138.B364
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1963LU02      Bull.Am.Phys.Soc. 8, No.1, 60, R6 (1963)

E.J.Ludwig, D.W.Miller

Proton Polarization in the Sr88(d, p)Sr89* Reaction

NUCLEAR STRUCTURE 89Sr; measured not abstracted; deduced nuclear properties.


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