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NSR database version of April 27, 2024.

Search: Author = S.Wustenbecker

Found 8 matches.

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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

1987SE13      Nucl.Instrum.Methods Phys.Res. A260, 33 (1987)

S.Seuthe, H.W.Becker, A.Krauss, A.Redder, C.Rolfs, U.Schroder, H.P.Trautvetter, K.Wolke, S.Wustenbecker, R.W.Kavanagh, F.B.Waanders

Production and Properties of Implanted Targets

NUCLEAR REACTIONS, ICPND ¹²C(p, γ), E=220-340 keV; ¹²C(α, γ), E=2.65-2.85 MeV; ¹⁴N(p, γ), E=260-360 keV; ²⁰Ne(p, γ), E=1165-1185 keV; ²³Na(p, γ), E=300-400 keV; measured γ-ray yields. Implanted targets.

doi: 10.1016/0168-9002(87)90385-8
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