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NSR database version of April 27, 2024.

Search: Author = M.Buschmann

Found 6 matches.

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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.