NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = W.H.Schulte Found 32 matches. 2000HA62 Eur.Phys.J. A 9, 479 (2000) S.Harissopulos, C.Chronidou, K.Spyrou, T.Paradellis, C.Rolfs, W.H.Schulte, H.W.Becker The 27Al(p, γ)28Si Reaction: Direct capture cross-section and resonance strengths at Ep = 0.2-1.12 MeV NUCLEAR REACTIONS 27Al(p, γ), E=200-1155 keV; measured Eγ, Iγ, sum-energy, thick target yields, capture σ; deduced resonance strengths, astrophysical S-factors.
doi: 10.1007/s100500070006
2000SP04 Eur.Phys.J. A 7, 79 (2000) K.Spyrou, C.Chronidou, S.Harissopulos, S.Kossionides, T.Paradellis, C.Rolfs, W.H.Schulte, L.Borucki Cross Section and Resonance Strength Measurements of 19F(p, αγ)16O at Ep = 200-800 keV NUCLEAR REACTIONS 19F(p, α), E=200-800 keV; measured Eγ, Iγ; deduced excitation function, resonances, strengths, widths, astrophysical S-factors, reaction rates.
doi: 10.1007/s100500050014
1999BO29 Eur.Phys.J. A 5, 327 (1999) L.Borucki, H.W.Becker, F.Gorris, S.Kubsky, W.H.Schulte, C.Rolfs Hydrogen Doppler Spectroscopy using 15N Ions NUCLEAR REACTIONS 20,22Ne(p, γ), 4He(7Li, γ), (11B, γ), (14N, γ), (16O, γ), E not given; measured resonance γ-ray yields; deduced atomic, molecular beams energy spreads. 20Ne(p, p), (p, p'), E=3552 keV; measured proton spectra; deduced resonance features.
doi: 10.1007/s100500050291
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
1998VA14 Nucl.Instrum.Methods Phys.Res. B136-138, 72 (1998) H.van Bebber, L.Borucki, K.Farzin, A.Z.Kiss, W.H.Schulte Total Cross Section of the 14N(d, pγ)15N Nuclear Reaction for Analytical Applications NUCLEAR REACTIONS 14N(d, p), E=500-1500 keV; measured γ-spectra; deduced total σ. NaI bore hole detector.
doi: 10.1016/S0168-583X(97)00672-1
1997GR11 Nucl.Phys. A621, 603c (1997) U.Greife, C.Arpesella, E.Bellotti, K.Brand, C.Broggini, L.Campajola, P.Corvisiero, A.D'Onofrio, G.Fiorentini, A.Fubini, G.Gervino, L.Gialanella, C.Gustavino, E.Huttel, M.Junker, R.W.Kavanagh, R.Kubat, J.Lambert, G.Oliviero, P.Prati, H.Rebel, V.Roca, W.S.Rodney, C.Rolfs, M.Romano, M.Romoli, S.Schmidt, W.H.Schulte, F.Strieder, F.Terrasi, H.P.Trautvetter, D.Zahnow, S.Zavatarelli Further Direct Approaches to the Nuclear Reactions in the Sun
doi: 10.1016/S0375-9474(97)00312-6
1997ST19 Nucl.Phys. A621, 123c (1997) F.Strieder, L.Campajola, A.D'Onofrio, L.Gialanella, U.Greife, V.Roca, C.Rolfs, M.Romano, M.Romoli, S.Schmidt, W.H.Schulte, H.P.Trautvetter, D.Zahnow The d(7Li, p)8Li Cross Section Near E(cm) = 0.61 MeV NUCLEAR REACTIONS, ICPND 2H(7Li, 8Li), E=0.47-4 MeV; measured recoil β-delayed α-decay spectra; deduced σ.
doi: 10.1016/S0375-9474(97)00222-4
1996BB22 Nucl.Instrum.Methods Phys.Res. B118, 499 (1996) I.J.R.Baumvol, L.Borucki, J.Chaumont, J.-J.Ganem, O.Kaytasov, N.Piel, S.Rigo, W.H.Schulte, F.C.Stedile, I.Trimaille Isotopic Tracing of Si During Thermal Growth of Si3N4 Ultrathin Films NUCLEAR REACTIONS 29Si(p, γ), E ≈ 324 keV; measured Eγ, Iγ; deduced σ.
doi: 10.1016/0168-583X(95)01478-0
1996CA43 Z.Phys. A356, 107 (1996) L.Campajola, L.Gialanella, K.Brand, A.D'Onofrio, U.Greife, E.Huttel, R.Kubat, G.Oliviero, H.Rebel, V.Roca, C.Rolfs, M.Romano, M.Romoli, S.Schmidt, W.H.Schulte, F.Strieder, F.Terrasi, H.-P.Trautvetter, D.Zahnow Production of an 8.0 MeV 7Be Ion Beam at the Naples TTT-3 Accelerator NUCLEAR REACTIONS 1H(7Be, γ), E=8 MeV; measured residual nuclei production. Radioactive beam from 7Li(p, n) reaction.
doi: 10.1007/s002180050154
1996GI11 Nucl.Instrum.Methods Phys.Res. A376, 174 (1996) L.Gialanella, F.Strieder, K.Brand, L.Campajola, A.D'Onofrio, U.Greife, E.Huttel, F.Petrazzuolo, V.Roca, C.Rolfs, M.Romano, M.Romoli, S.Schmidt, W.H.Schulte, F.Terrasi, H.P.Trautvetter, D.Zahnow A Recoil Separator for the Measurement of Radiative Capture Reactions NUCLEAR REACTIONS 1H(12C, γ), E=2, 11 MeV; measured Eγ, Iγ; deduced absolute reaction σ. Recoil separator plus windowless gas target.
doi: 10.1016/0168-9002(96)00264-1
1996PI15 Nucl.Instrum.Methods Phys.Res. B118, 186 (1996) N.Piel, W.H.Schulte, M.Berheide, H.W.Becker, L.Borucki, C.Grama, M.Mehrhoff, C.Rolfs Efficient γ-Ray Detection in Ion Beam Analysis NUCLEAR REACTIONS 29Si(p, γ), E=325, 420 MeV; measured Eγ, Iγ; deduced resonance yields.
doi: 10.1016/0168-583X(95)01453-5
1996ST08 Nucl.Phys. A601, 168 (1996) F.Stegmuller, C.Rolfs, S.Schmidt, W.H.Schulte, H.P.Trautvetter, R.W.Kavanagh 22Na(p, γ)23Mg Resonant Reaction at Low Energies NUCLEAR REACTIONS 22Na(p, γ), E=0.2-0.63 MeV; measured γ-spectra; deduced reaction rates. 23Mg deduced resonance energies, resonance strengths, reaction rates.
doi: 10.1016/0375-9474(96)00084-X
1996ST18 Z.Phys. A355, 209 (1996) F.Strieder, L.Gialanella, U.Greife, C.Rolfs, S.Schmidt, W.H.Schulte, H.P.Trautvetter, D.Zahnow, F.Terrasi, L.Campajola, A.D'Onofrio, V.Roca, M.Romano, M.Romoli The d(7Li, p)8Li Cross Section Near E(cm) = 0.61 MeV NUCLEAR REACTIONS, ICPND 2H(7Li, p), E(cm) ≈ 0.61 MeV; measured proton yield, β-delayed α-activity of residual 8Li. 2H(7Li, p), E(cm)=0.5-0.75 MeV; measured σ(θ); deduced absolute σ(E), consequences for expected flux of high energy solar neutrinos.
doi: 10.1007/s002180050100
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
1995SC36 Nucl.Phys. A591, 227 (1995) S.Schmidt, C.Rolfs, W.H.Schulte, H.P.Trautvetter, R.W.Kavanagh, C.Hategan, S.Faber, B.D.Valnion, G.Graw 22Na(3He, d)23Mg Reaction Studies of States Near the Proton Threshold and Hydrogen Burning of 22Na NUCLEAR REACTIONS 22Na(3He, d), E=30 MeV; measured deuteron spectra, σ(θ); deduced stellar reaction rates. 23Mg deduced resonances, J, π, Γ(p), resonance strengths. DWBA analysis.
doi: 10.1016/0375-9474(95)00164-V
1995ZA03 Z.Phys. A351, 229 (1995) D.Zahnow, C.Angulo, C.Rolfs, S.Schmidt, W.H.Schulte, E.Somorjai The S(E) Factor of 7Li(p, γ)8Be and Consequences for S(E) Extrapolation in 7Be(p, γ0)8B NUCLEAR REACTIONS, ICPND 7Li(p, γ), E=100-1500 keV; measured Eγ, Iγ(θ) ratios; deduced σ(E), astrophysical S-factor vs E, capture mechanism. 8Be deduced resonance energy, Γ.
doi: 10.1007/BF01289534
1995ZA04 Nucl.Phys. A589, 95 (1995) D.Zahnow, C.Angulo, M.Junker, C.Rolfs, S.Schmidt, W.H.Schulte, E.Somorjai Thermonuclear Reaction Rates of 9Be(p, γ)10B NUCLEAR REACTIONS, ICPND 9Be(p, γ), E=75-1800 keV; measured Eγ, Iγ; deduced σ(E), thermonuclear reaction rates, astrophysical S-factor.
doi: 10.1016/0375-9474(95)00077-E
1994BA86 Nucl.Instrum.Methods Phys.Res. B85, 326 (1994) G.Battistig, G.Amsel, I.Trimaille, J.-J.Ganem, S.Rigo, F.C.Stedile, I.J.R.Baumvol, W.H.Schulte, H.W.Becker High Resolution Low Energy Resonance Depth Profiling of 18O in Near Surface Isotopic Tracing Studies NUCLEAR REACTIONS 18O(p, α), E ≈ resonance; measured σ(E); deduced Si oxidation processes features. Depth profiling of 18O, near surface isotopic training.
doi: 10.1016/0168-583X(94)95837-8
1994BO52 Nucl.Instrum.Methods Phys.Res. B89, 8 (1994) G.Bogaert, R.Meunier, D.Ledu, C.Angulo, W.H.Schulte, P.Aguer, A.Coc, A.Lefebvre, F.de Oliveira, J.P.Thibaud, T.Paradellis, E.Kossionides, S.Harissopulos, G.Galios A 250 kV High Current Ion Accelerator for Applications in Nuclear Astrophysics NUCLEAR REACTIONS, ICPND 24Mg(p, γ), E ≈ 223 keV; measured thick target yield curve; deduced ion accelerator energy spread, stability.
doi: 10.1016/0168-583X(94)95135-7
1994GR33 Nucl.Instrum.Methods Phys.Res. A350, 327 (1994) U.Greife, C.Arpesella, C.A.Barnes, F.Bartolucci, E.Bellotti, C.Broggini, P.Corvisiero, G.Fiorentini, A.Fubini, G.Gervino, F.Gorris, C.Gustavino, M.Junker, R.W.Kavanagh, A.Lanza, G.Mezzorani, P.Prati, P.Quarati, W.S.Rodney, C.Rolfs, W.H.Schulte, H.P.Trautvetter, D.Zahnow Laboratory for Underground Nuclear Astrophysics (LUNA) NUCLEAR REACTIONS, ICPND 2H(d, n), (d, p), E=10 keV; 2H(3He, p), E=70 keV; measured spectra. 2H(3He, p), E ≤ 40 keV; 3He(3He, 2p), E ≤ 160 keV; measured astrophysical S-factor vs E. Windowless gas target system, close geometry detector telescopes.
doi: 10.1016/0168-9002(94)91182-7
1994PR09 Z.Phys. A350, 171 (1994) P.Prati, C.Arpesella, F.Bartolucci, H.W.Becker, E.Bellotti, C.Broggini, P.Corvisiero, G.Fiorentini, A.Fubini, G.Gervino, F.Gorris, U.Greife, C.Gustavino, M.Junker, C.Rolfs, W.H.Schulte, H.P.Trautvetter, D.Zahnow Electron Screening in the d + 3He Fusion Reaction NUCLEAR REACTIONS, ICPND 2H(3He, p), E(cm)=5.4-31.3 keV; measured spectra, astrophysical S-factor; deduced electron screening potential. Windowless gas target system.
doi: 10.1007/BF01290685
1994ST13 Nucl.Instrum.Methods Phys.Res. B85, 248 (1994) F.C.Stedile, I.J.R.Baumvol, J.-J.Ganem, S.Rigo, I.Trimaille, G.Battistig, W.H.Schulte, H.W.Becker IBA Study of the Growth Mechanisms of Very Thin Silicon Oxide Films: The effect of wafer cleaning NUCLEAR REACTIONS 16,18O(α, α), E=1.8 MeV; measured Rutherford backscattering spectra; deduced very thin Si oxide films growth mechanisms features. Isotopic profiles from ion beam analysis methods.
doi: 10.1016/0168-583X(94)95821-1
1993AN06 Z.Phys. A345, 231 (1993) C.Angulo, S.Engstler, G.Raimann, C.Rolfs, W.H.Schulte, E.Somorjai The Effects of Electron Screening and Resonances in (p, α) Reactions on 10B and 11B at Thermal Energies NUCLEAR REACTIONS, ICPND 11,10B(p, α), E(cm)=17-134 keV; measured spectra, α yield. 11B(p, γ), E=140-260 keV; 1H(19F, αγ), E ≈ 6.23-7.83; measured thick target yield; deduced absolute astrophysical S-factor vs E, electron screening role.
doi: 10.1007/BF01293350
1993AN09 Z.Phys. A345, 333 (1993) C.Angulo, W.H.Schulte, D.Zahnow, G.Raimann, C.Rolfs Astrophysical S(E) Factor of 10B(p, α1)7Be at Low Energies NUCLEAR REACTIONS, ICPND 10B(p, α), E(cm)=48-159 keV; measured absolute fusion σ, astrophysical S-factor vs E. γ-spectroscopic techniques.
doi: 10.1007/BF01280844
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.
1990SE09 Nucl.Phys. A514, 471 (1990) S.Seuthe, C.Rolfs, U.Schroder, W.H.Schulte, E.Somorjai, H.P.Trautvetter, F.B.Waanders, R.W.Kavanagh, H.Ravn, M.Arnould, G.Paulus Resonances in the 22Na(p, γ)23Mg Reaction NUCLEAR REACTIONS, ICPND 22Na(p, γ), E=0.17-1.29 MeV; measured γ-spectra; deduced stellar reaction rates. 23Mg deduced resonances, resonance strengths.
doi: 10.1016/0375-9474(90)90153-D
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
1986FR18 J.Phys.(London) B19, 2907 (1986) R.Frekers, H.Schulze, W.-H.Schulte, B.Cleff Threshold Behaviour of L-Shell Ionisation in Slow Symmetric Ion-Atom Collisions with 32 ≤ Z ≤ 54 ATOMIC MASSES Ge(Ge, X), Kr(Kr, X), In(In, X), Mo(Mo, X), Xe(Xe, X), E=0.05-3 MeV; measured X-ray yield; deduced total L-shell ionization σ, multiple collision influence, ionization threshold behaviour. Si-Li detector. Coupled, simplified state calculations.
doi: 10.1088/0022-3700/19/18/020
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