NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = G.Roters Found 6 matches. 1999RO24 Eur.Phys.J. A 6, 451 (1999) G.Roters, C.Rolfs, F.Strieder, H.P.Trautvetter The E1 and E2 Capture Amplitudes in 12C(α, γ0)16O NUCLEAR REACTIONS 4He(12C, γ), E=0.94-3.4 MeV; measured Eγ, Iγ, excitation function; deduced E1, E2 contributions.
doi: 10.1007/s100500050369
1997TR07 Nucl.Phys. A621, 161c (1997) H.P.Trautvetter, G.Roters, C.Rolfs, S.Schmidt, P.Descouvemont The E2-Contribution to the 12C(α, γ)16O-Reaction NUCLEAR REACTIONS, ICPND 4He(12C, γ), E=0.9-3.4 MeV; measured Eγ, Iγ; deduced astrophysical S-factors vs E for E1, E2 transitions. Other data considered.
doi: 10.1016/S0375-9474(97)00230-3
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
1994IL01 Nucl.Phys. A571, 132 (1994) C.Iliadis, J.Gorres, J.G.Ross, K.W.Scheller, M.Wiescher, R.E.Azuma, G.Roters, H.P.Trautvetter, H.C.Evans Explosive Hydrogen Burning of 35Cl NUCLEAR REACTIONS 35Cl(3He, d), E=15 MeV; measured σ(θ), σ(Ed). 32S(6Li, d), E=32 MeV; measured σ(Ed). 32S(α, γ), E ≈ resonance; measured Eγ, Iγ. 35Cl(p, γ), E ≈ 200-800 keV; measured γ yield vs E , stellar rates. 35Cl(p, X), E=177 keV; measured particle spectra. 36Ar deduced levels, J, π, L, spectroscopic factors, γ-branching ratios, resonance strengths. Deduced no evidence for (p, α) reactions.
doi: 10.1016/0375-9474(94)90345-X
1992BE45 Nucl.Instrum.Methods Phys.Res. A321, 521 (1992) M.Benjelloun, Th.Delbar, W.Galster, P.Leleux, E.Lienard, P.Lipnik, P.Duhamel, J.Vanhorenbeeck, C.Rolfs, G.Roters, H.P.Trautvetter, W.Rodney Precise Measurement of the J(π) = 1- Resonance in 14N by 13C + p Elastic Scattering on a Thick Target NUCLEAR REACTIONS 1H(13C, 13C), E=6.8-9.6 MeV; measured proton spectra. 14N deduced resonance energy, Γ. Proton, projectile energy loss, straggling considered correctly, thick CH2 target.
doi: 10.1016/0168-9002(92)90062-9
1991GA22 Phys.Rev. C44, 2776 (1991) W.Galster, P.Leleux, I.Licot, E.Lienard, P.Lipnik, D.Mertens, T.Delbar, J.Vervier, P.Decrock, M.Huyse, P.Van Duppen, P.Duhamel, J.Vanhorenbeeck, G.Roters, C.Rolfs, U.Schroeder, H.P.Trautvetter, K.Wolke, J.Lambert, W.S.Rodney Target and Detection Techniques for the 13N(p, γ)14O Reaction Using Radioactive Ion Beams: 13C(p, γ)14N reaction as a test case NUCLEAR REACTIONS, ICPND 1H(13C, 13C), (13C, γ), E(cm)=0.46-0.6 MeV; measured σ(E), thick target γ yield. 13C(p, γ), E=0.45-0.65 MeV; measured σ(E), thin targets. 14N deduced resonance, Γ, Γγ. Breit-Wigner analysis. Techniques for radioactive beams, gas, foil targets.
doi: 10.1103/PhysRevC.44.2776
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