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NSR database version of April 11, 2024.

Search: Author = J.S.Schweitzer

Found 21 matches.

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2006CA05      Phys.Rev. C 73, 014319 (2006)

E.Casarejos, C.Angulo, P.J.Woods, F.C.Barker, P.Descouvemont, M.Aliotta, T.Davinson, P.Demaret, M.Gaelens, P.Leleux, Z.Liu, M.Loiselet, A.S.Murphy, A.Ninane, I.A.Roberts, G.Ryckewaert, J.S.Schweitzer, F.Vanderbist

Low-lying states in the unbound 11N nucleus

NUCLEAR REACTIONS 1H(10C, p), E=25.5, 32 MeV; measured recoil Ep, elastic σ(θ). 11N deduced resonance parameters. 12O deduced two-proton decay width.

doi: 10.1103/PhysRevC.73.014319
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1513.


2003AN02      Phys.Rev. C 67, 014308 (2003)

C.Angulo, G.Tabacaru, M.Couder, M.Gaelens, P.Leleux, A.Ninane, F.Vanderbist, T.Davinson, P.J.Woods, J.S.Schweitzer, N.L.Achouri, J.C.Angelique, E.Berthoumieux, F.De Oliveira Santos, P.Himpe, P.Descouvemont

Identification of a new low-lying state in the proton drip line nucleus 19Na

NUCLEAR REACTIONS 1H(18Ne, 18Ne), E=21, 23.5, 28 MeV; measured recoil proton spectra, σ(θ). 19Na deduced level, J, π, width. Global R-matrix fit.

doi: 10.1103/PhysRevC.67.014308
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0347. Data from this article have been entered in the XUNDL database. For more information, click here.


2003AN28      Nucl.Phys. A719, 201c (2003)

C.Angulo, P.Descouvemont, M.Couder, M.Gaelens, P.Leleux, A.Ninane, G.Tabacaru, F.Vanderbist, T.Davinson, Ph.J.Woods, J.S.Schweitzer, N.L.Achouri, J.C.Angelique, E.Berthoumieux, F.de Oliveira Santos, P.Himpe

Spectroscopy of the proton drip line nucleus 19Na by 1H(18Ne, p)18Ne elastic scattering

NUCLEAR REACTIONS 1H(18Ne, p), E=21, 23.5, 28 MeV; measured recoil proton spectra, elastic σ(θ). 19Na deduced level energy, width.

doi: 10.1016/S0375-9474(03)00917-5
Citations: PlumX Metrics


1998BE71      Phys.Rev. B58, 11103 (1998)

M.Berheide, W.H.Schulte, H.-W.Becker, L.Borucki, M.Buschmann, N.Piel, C.Rolfs, G.E.Mitchell, J.S.Schweitzer

Average Kinetic Energy of Atoms in a Solid Measured with Resonant Nuclear Reactions

NUCLEAR REACTIONS 21Ne(p, γ), E ≈ 272 keV; measured thick target yield curves; deduced target atoms average kinetic energy.

doi: 10.1103/PhysRevB.58.11103
Citations: PlumX Metrics


1995BE29      Z.Phys. A351, 453 (1995)

H.W.Becker, M.Bahr, M.Berheide, L.Borucki, M.Buschmann, C.Rolfs, G.Roters, S.Schmidt, W.H.Schulte, G.E.Mitchell, J.S.Schweitzer

Hydrogen Depth Profiling using 18O Ions

NUCLEAR REACTIONS, ICPND 1H(15N, α), E=6.58 MeV; 1H(18O, α), E=2.9 MeV; measured spectra. 18O(p, α), E ≈ 140-160 keV; calculated astrophysical S-factor vs E. 1H(15N, α), E ≈ 6.525-6.625 MeV; 1H(18O, α), E ≈ 2.85-2.95 MeV; measured yield ratio Iα/I(H) vs E. 16O, 19F deduced more accurate resonance parameters. 1H(18O, α), E ≈ 2.68-2.78 MeV; measured α-yield vs E. 1H(15N, α), E ≈ 6.36-6.48 MeV; measured γ yield vs E. Single stage accelerator technique, depth profiling applications.

doi: 10.1007/BF01291151
Citations: PlumX Metrics


1992BE35      Z.Phys. A343, 361 (1992)

H.W.Becker, H.Ebbing, W.H.Schulte, S.Wustenbecker, M.Berheide, M.Buschmann, C.Rolfs, G.E.Mitchell, J.S.Schweitzer

Low Energy Resonances in 21Ne(p, γ)22Na Examined with a High Energy Resolution Ion Beam

NUCLEAR REACTIONS, ICPND 21Ne(p, γ), E ≈ resonance; measured γ yield. 22Na deduced resonance structure, widths. High energy resolution ion beam.

doi: 10.1007/BF01291537
Citations: PlumX Metrics


1992SC08      Nucl.Instrum.Methods Phys.Res. B64, 383 (1992)

W.H.Schulte, H.Ebbing, H.W.Becker, S.Wustenbecker, M.Berheide, M.Buschmann, C.Rolfs, G.E.Mitchell, J.S.Schweitzer

Measurement and Analysis of Thin- and Thick-Target Yield Curves of Narrow Resonances with a High Energy Resolution Ion Beam

NUCLEAR REACTIONS, ICPND 21Ne(p, γ), E ≈ resonance; measured γ yield curve; deduced atomic effects role. Thin, thick targets.

doi: 10.1016/0168-583X(92)95500-Q
Citations: PlumX Metrics


1992SC27      Nucl.Instrum.Methods Phys.Res. B71, 291 (1992)

W.H.Schulte, H.Ebbing, S.Wustenbecker, H.W.Becker, M.Berheide, M.Buschmann, C.Rolfs, G.E.Mitchell, J.S.Schweitzer

High Energy Resolution Ion Beam Techniques for Novel Investigations in Nuclear, Atomic and Applied Physics Using Narrow Nuclear Resonances

NUCLEAR REACTIONS, ICPND 23Na, 21Ne(p, γ), E ≈ resonance; measured γ yield vs E. High energy resolution ion beam techniques.

doi: 10.1016/0168-583X(92)95401-C
Citations: PlumX Metrics


1992WU09      Z.Phys. A344, 205 (1992)

S.Wustenbecker, H.W.Becker, H.Ebbing, W.H.Schulte, M.Berheide, M.Buschmann, C.Rolfs, G.E.Mitchell, J.S.Schweitzer

Atomic Effects on α-α Scattering to the 8Be Ground State

NUCLEAR REACTIONS 4He(α, α), E ≈ resonance; measured relative yield; deduced 8Be resonance splitting mechanism, astrophysical significance. Crossing beams technique.


1989WU03      Nucl.Instrum.Methods Phys.Res. B40/41, 413 (1989)

S.Wustenbecker, W.H.Schulte, H.Ebbing, H.Baumeister, H.W.Becker, B.Cleff, C.Rolfs, H.P.Trautvetter, G.E.Mitchell, J.S.Schweitzer, C.A.Peterson

Technical Improvements for High Resolution Ion Beam Experiments

NUCLEAR REACTIONS 23Na(p, γ), E ≈ 309 keV; 27Al(p, γ), E ≈ 327 keV; measured thick target γ yield curve.

doi: 10.1016/0168-583X(89)91010-0
Citations: PlumX Metrics


1989WU06      Nucl.Instrum.Methods Phys.Res. A279, 448 (1989)

S.Wustenbecker, H.Ebbing, W.H.Schulte, H.Baumeister, H.W.Becker, B.Cleff, C.Rolfs, H.P.Trautvetter, G.E.Mitchell, J.S.Schweitzer, C.A.Peterson

Improvements in Targetry and High Voltage Stability for High Resolution Ion Beam Experiments

NUCLEAR REACTIONS 23Na(p, γ), E=0.309 MeV; 21Ne(p, γ), E ≈ 0.272 MeV; 26Mg(p, γ), E=0.338 MeV; 27Al(p, γ), E=0.327 MeV; measured thick target γ-yield vs E. High resolution ion beams, energies around resonances.

doi: 10.1016/0168-9002(89)91292-8
Citations: PlumX Metrics


1987WU04      Nucl.Instrum.Methods Phys.Res. A256, 9 (1987)

S.Wustenbecker, H.W.Becker, C.Rolfs, H.P.Trautvetter, K.Brand, G.E.Mitchell, J.S.Schweitzer

Technical Developments for Ion Beams with High Energy Resolution

NUCLEAR REACTIONS 27Al(p, γ), E ≈ 992 keV; 20Ne, 18O(p, γ), E ≈ 1167 keV; measured γ-yields; deduced beam energy stability, oscillator frequency dependences.

doi: 10.1016/0168-9002(87)91034-5
Citations: PlumX Metrics


1977SC24      Nucl.Phys. A287, 344 (1977)

J.S.Schweitzer, Z.E.Switkowski, R.M.Wieland

Low-Energy Proton Reactions on 45Sc of Interest in Stellar Nucleosynthesis

NUCLEAR REACTIONS 45Sc(p, p'), 45Sc(p, α), E=2.5-3.8 MeV; measured σ(E:Ep', θ), σ(E:Eα, θ). Natural targets. Hauser-Feshbach analysis.

doi: 10.1016/0375-9474(77)90500-0
Citations: PlumX Metrics


1976IN01      Phys.Rev. C13, 524 (1976)

P.D.Ingalls, J.S.Schweitzer, B.D.Anderson, M.Rios

14N(p, α)11C Cross Sections from 3.8 to 6.4 MeV

NUCLEAR REACTIONS 14N(p, α), E=3.8-6.4 MeV; measured σ(E). Inferred σ(E), astrophysical σ factor for inverse reaction. Sealed gas target.

doi: 10.1103/PhysRevC.13.524
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0178.


1976LO03      Nucl.Phys. A259, 122 (1976)

M.Lowry, J.S.Schweitzer, R.Dayras, R.G.Stokstad

Cross Sections for 6Li Production in the Reactions 10B + 16O and 12C + 14N at Low Energies

NUCLEAR REACTIONS 10B(16O, 6Li), E(cm)=7.5-16.15 MeV; 12C(14N, 6Li), E(cm)=13.8-16.6 MeV; measured σ(θ). 20Ne deduced levels. Hauser-Feshbach analysis.

doi: 10.1016/0375-9474(76)90499-1
Citations: PlumX Metrics


1974AN19      Nucl.Phys. A233, 286 (1974)

B.D.Anderson, M.R.Dwarakanath, J.S.Schweitzer, A.V.Nero

A New Determination of the Partial Widths of the 16.11 MeV State in 12C

NUCLEAR REACTIONS 11B(d, n), E=6 MeV; measured σ(En, θ); 11B(p, γ), (p, α), E=163 keV; measured σ; 10B(3He, pγ), E=2.2 MeV; measured pγ-coin. 12C levels deduced p-width, γ-width, S.

doi: 10.1016/0375-9474(74)90456-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0359.


1974RI16      Nucl.Phys. A236, 523 (1974)

M.Rios, B.D.Anderson, J.S.Schweitzer

The 46Ti(p, γ)47V, 50Cr(p, γ)51Mn, 58Ni(α, γ)62Zn and 58Ni(α, p)61Cu Cross Sections

NUCLEAR REACTIONS 46Ti, 50Cr(p, γ), 58Ni(α, γ), (α, p); measured σ(E). Natural, enriched targets.

doi: 10.1016/0375-9474(74)90271-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1111.


1973SC02      Nucl.Phys. A199, 424 (1973)

J.S.Schweitzer, P.C.Simms

Energy-Dependent β-γ Circular Polarization and Nuclear Matrix Elements in 84Rb

RADIOACTIVITY 84Rb; measured βγ-circular polarization; deduced nuclear matrix elements.

doi: 10.1016/0375-9474(73)90559-9
Citations: PlumX Metrics


1973SC06      Nucl.Phys. A202, 602 (1973)

J.S.Schweitzer, P.C.Simms

Nuclear Matrix Elements in the First-Forbidden β-Decay of 125Sb

RADIOACTIVITY 125Sb measured nothing; 125Te deduced nuclear matrix elements in β-decay.

doi: 10.1016/0375-9474(73)90646-5
Citations: PlumX Metrics


1973SM07      Nucl.Phys. A211, 473 (1973)

H.A.Smith, Jr., J.S.Schweitzer, P.C.Simms

Nuclear Matrix Elements in the First-Forbidden β-Decays of 122Sb and 124Sb

RADIOACTIVITY 122,124Sb; deduced β-decay, nuclear matrix elements.

doi: 10.1016/0375-9474(73)90437-5
Citations: PlumX Metrics


1972SC43      Nucl.Phys. A198, 481 (1972)

J.S.Schweitzer, P.C.Simms

A Comparison of Methods for Determining Nuclear Matrix Elements in First-Forbidden β-Decay

RADIOACTIVITY 198Au; analyzed βγ(θ), βγ-CP, β-shape factor; deduced nuclear matrix elements.

doi: 10.1016/0375-9474(72)90703-8
Citations: PlumX Metrics


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