NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Schweitzer Found 23 matches. 2018ZI03 Phys.Rev. C 97, 065806 (2018) J.Zickefoose, A.Di Leva, F.Strieder, L.Gialanella, G.Imbriani, N.De Cesare, C.Rolfs, J.Schweitzer, T.Spillane, O.Straniero, F.Terrasi Measurement of th e 12C(12C, p)23Na cross section near the Gamow energy NUCLEAR REACTIONS 12C(12C, p), E=2.00-4.00 MeV; measured Ep, Ip, thick-target yields at CIRCE, Vanvitelli accelerator facility; deduced astrophysical S-factor for p0 and p1 channels, proton-channel to total S-factor ratio, resonance strength at 2.1 MeV, and constrained potential resonance strength at 1.5 MeV. Comparison with previous experimental, and with potential model calculations.
doi: 10.1103/PhysRevC.97.065806
2007SP03 Phys.Rev.Lett. 98, 122501 (2007) T.Spillane, F.Raiola, C.Rolfs, D.Schurmann, F.Strieder, S.Zeng, H.-W.Becker, C.Bordeanu, L.Gialanella, M.Romano, J.Schweitzer 12C + 12C Fusion Reactions near the Gamow Energy NUCLEAR REACTIONS 12C(12C, p), (12C, α), E=2.1-4.75 MeV; measured Eγ, Iγ; deduced σ, astrophysical S-factors, resonance features.
doi: 10.1103/PhysRevLett.98.122501
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1973SC02 Nucl.Phys. A199, 424 (1973) 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
1973SC06 Nucl.Phys. A202, 602 (1973) 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
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
1972SC43 Nucl.Phys. A198, 481 (1972) 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
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