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NSR database version of May 19, 2024.

Search: Author = W.Bohne

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2001LO04      Phys.Rev. C63, 034616 (2001)

B.Lott, F.Goldenbaum, A.Bohm, W.Bohne, T.von Egidy, P.Figuera, J.Galin, D.Hilscher, U.Jahnke, J.Jastrzebski, M.Morjean, G.Pausch, A.Peghaire, L.Pienkowski, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid

Thermal Excitation and Decay of Nuclei from Antiproton-Nucleus Interactions at 1.22 GeV

NUCLEAR REACTIONS 12C, Cu, Y, 92,100Mo, 107Ag, Sn, 165Ho, 197Au, Bi, 238U(p-bar, X), E=1.22 GeV; measured light charged particle, intermediate mass fragment, neutron multiplicities, spectra, excitation energy distributions. 197Au, 238U(p-bar, X), E=1.22 GeV; measured fission probability, fragment kinetic energy distributions. Comparisons with model predictions.

doi: 10.1103/PhysRevC.63.034616
Citations: PlumX Metrics


2000PI02      Phys.Lett. 472B, 15 (2000)

L.Pienkowski, W.Bohne, T.von Egidy, P.Figuera, J.Galin, F.Goldenbaum, D.Hilscher, U.Jahnke, J.Jastrzebski, B.Lott, M.Morjean, G.Pausch, A.Peghaire, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid

Vaporization and Multifragmentation in the Reaction 1.2 GeV (p-bar) + Cu and Ag

NUCLEAR REACTIONS Cu, Ag(p-bar, X), E=1.2 GeV; measured particle energy, (particle)(particle)-coin, excitation energy and mass distributions, particle multiplicities, ratio of vaporization to reaction σ. Intranuclear cascade and statistical model calculations.

doi: 10.1016/S0370-2693(99)01410-0
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1999JA14      Phys.Rev.Lett. 83, 4959 (1999)

U.Jahnke, W.Bohne, T.von Egidy, P.Figuera, J.Galin, F.Goldenbaum, D.Hilscher, J.Jastrzebski, B.Lott, M.Morjean, G.Pausch, A.Peghaire, L.Pienkowski, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid

Prevalence of Fission and Evaporation in the Decay of Heavy Nuclei Excited Up to 1000 MeV with Energetic Antiprotons

NUCLEAR REACTIONS 165Ho, 197Au, 238U(p-bar, X), E=1.22 GeV; measured fission fragments, heavy residues kinetic energy vs excitation energy, intermediate mass fragments multiplicity; deduced fission, heavy residue production probabilities. Comparison with statistical model.

doi: 10.1103/PhysRevLett.83.4959
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1999LO22      Nucl.Phys. (Supplement) A654, 803c (1999)

B.Lott, W.Bohne, J.Eades, T.von Egidy, P.Figuera, H.Fuchs, J.Galin, K.Gulda, F.Goldenbaum, D.Hilscher, U.Jahnke, J.Jastrzebski, W.Kurcewicz, M.Morjean, G.Pausch, A.Peghaire, L.Pienkowski, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid, P.Ziem

Formation and Decay of Nuclei Heated with High-Energy Antiprotons

NUCLEAR REACTIONS 197Au, 238U(p-bar, X), E=1.22 GeV; measured fission probability and intermediate mass fragment vs excitation energy. Absence of multifragmentation discussed.

doi: 10.1016/S0375-9474(00)88550-4
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1999PI10      Nucl.Phys. A655, 269c (1999)

L.Pienkowski, W.Bohne, J.Eades, T.von Egidy, P.Figuera, H.Fuchs, J.Galin, F.Goldenbaum, Ye.S.Golubeva, K.Gulda, D.Hilscher, A.S.Iljinov, U.Jahnke, J.Jastrzebski, W.Kurcewicz, B.Lott, M.Morjean, G.Pausch, A.Peghaire, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid, P.Ziem

Decay of Hot Nuclei Formed with Energetic Antiprotons (PS208)

NUCLEAR REACTIONS Ho, 197Au, U(p-bar, X), E=1.22 GeV; measured neutron multiplicity, fragment mass distributions, fission probability.

doi: 10.1016/S0375-9474(99)00212-2
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1997SC27      Z.Phys. A359, 27 (1997)

S.Schmid, W.Schmid, F.J.Hartmann, T.von Egidy, D.Hilscher, W.Bohne, P.Figuera, F.Goldenbaum, U.Jahnke, D.Polster, P.Ziem, J.Galin, B.Lott, M.Morjean, A.Peghaire, B.Quednau, K.Gulda, J.Jastrzebski, W.Kurcewicz, L.Pienkowski, G.Pausch, J.Eades, A.S.Iljinov, M.V.Mebel

Probability of Fission Induced by 1.2 GeV Antiprotons

NUCLEAR REACTIONS 238U, 232Th, 209Bi, 197Au, 165Ho, 119Sn, Ag, 100Mo, 89Y, Cu(p-bar, F), E=1.2 GeV; measured annihilation σ, absolute fission probability vs fragment mass, neutron multiplicity, fission fragment folding angle distributions. Monte Carlo calculations. 4π neutron, particle detectors.

doi: 10.1007/s002180050363
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1996GO25      Phys.Rev.Lett. 77, 1230 (1996)

F.Goldenbaum, W.Bohne, J.Eades, T.von Egidy, P.Figuera, H.Fuchs, J.Galin, Ye.S.Golubeva, K.Gulda, D.Hilscher, A.S.Iljinov, U.Jahnke, J.Jastrzebski, W.Kurcewicz, B.Lott, M.Morjean, G.Pausch, A.Peghaire, L.Pienkowski, D.Polster, S.Proschitzki, B.Quednau, H.Rossner, S.Schmid, W.Schmid, P.Ziem

Heating of Nuclei with Energetic Antiprotons

NUCLEAR REACTIONS Cu, Ho, 197Au, U(p-bar, X), E=1.2 GeV; measured neutron multiplicity vs charged particle multiplicity, excitation energy distribution; deduced nuclei decay mechanism.

doi: 10.1103/PhysRevLett.77.1230
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1995FI04      Z.Phys. A352, 315 (1995)

P.Figuera, W.Bohne, B.Drescher, F.Goldenbaum, D.Hilscher, U.Jahnke, B.Lott, L.Pienkowski, P.Ziem

Maximum Excitation Energy in Fusion-Evaporation Reactions from Light Particle Multiplicity Measurements in 32S + 58Ni at 25 MeV/A

NUCLEAR REACTIONS 58Ni(32S, X), E=25 MeV/nucleon; measured (light particle)(evaporation residue)-coin; deduced system maximum excitation energy.

doi: 10.1007/BF01289504
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1995PA48      Nucl.Instrum.Methods Phys.Res. A365, 176 (1995)

G.Pausch, M.Moszynski, D.Wolski, W.Bohne, H.Grawe, D.Hilscher, R.Schubart, G.de Angelis, M.de Poli

Application of the Pulse-Shape Technique to Proton-Alpha Discrimination in Si-Detector Arrays

NUCLEAR REACTIONS Ni(36Ar, X), E=150 MeV; measured light charged particle spectra; deduced detector characteristics. Reversed n-type Si detectors.

doi: 10.1016/0168-9002(95)00488-2
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1995VO14      Z.Naturforsch. 50a, 1077 (1995)

T.von Egidy, F.J.Hartmann, S.Schmid, W.Schmid, K.Gulda, J.Jastrzebski, W.Kurcewicz, P.Lubinski, L.Pienkowski, A.Trzcinska, D.Hilscher, W.Bohne, F.Goldenbaum, U.Jahnke, D.Polster, H.Rossner, A.S.Iljinov, D.I.Ivanov, M.V.Mebel, V.G.Nedorezov, A.S.Sudov, J.Eades, S.Neumaier

Nuclear Physics with Antiprotons

NUCLEAR REACTIONS 197Au(p-bar, X), E at rest; 197Au(p-bar, X), E=1.2 GeV; 197Au(p, X), E=1, 6 GeV; compiled, reviewed residuals yields vs mass number. 234U(p-bar, F), E at rest; 234U(p-bar, F), E=fast; measured neutron spectra following fission; deduced absolute fission probabilities.


1994PA43      Nucl.Instrum.Methods Phys.Res. A337, 573 (1994)

G.Pausch, W.Bohne, D.Hilscher

Particle Identification in Solid-State Detectors by Means of Pulse-Shape Analysis - Results of Computer Simulations

NUCLEAR REACTIONS Ho(12C, X), E=360 MeV; calculated fragment (charge sample)/energy deposition. 197Au(32S, X), E=795 MeV; measured charge balance parameter vs energy deposited; deduced Z identification suitability. Semi-empirical model.

doi: 10.1016/0168-9002(94)91129-0
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1994PA52      Nucl.Instrum.Methods Phys.Res. A349, 281 (1994)

G.Pausch, W.Bohne, D.Hilscher, H.-G.Ortlepp, D.Polster

Particle Identification in a Wide Dynamic Range Based on Pulse-Shape Analysis with Solid-State Detectors

NUCLEAR REACTIONS 197Au, Ni, C(32S, X), E=698 MeV; measured fragment count rate vs energy deposition; deduced detector charge resolution features. Planar Si detector.

doi: 10.1016/0168-9002(94)90634-3
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1994SZ07      Phys.Rev. C50, 3151 (1994)

A.Szanto de Toledo, E.M.Szanto, R.M.Anjos, W.Bohne, H.Morgenstern

Saturation Effects in the 10B + 11B Reaction at E/A = 11 MeV

NUCLEAR REACTIONS 11B(10B, X), E=110 MeV; measured fragment mass distributions, σ(evaporation residue); deduced saturation effects related features.

doi: 10.1103/PhysRevC.50.3151
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1993BO39      Z.Phys. A347, 135 (1993)

W.Bohne, P.Figuera, H.Morgenstern, S.Proschitzki

Limiting Excitation Energies in Fusion Evaporation Reactions

NUCLEAR REACTIONS 45Sc, 58Fe, 58Ni, 80Se, 92,100Mo(32S, X), E=710-960 MeV; measured evaporation residue mass width vs velocity, (light charged particle)(evaporation residue)-coin, other aspects; deduced critical excitation energy clear evidence.

doi: 10.1007/BF01284680
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1993MO02      Z.Phys. A344, 259 (1993)

H.Morgenstern, W.Bohne, S.Proschitzki

Particle Evaporation from Hot Nuclei with A ≤ 85 Mainly Prior to Scission

NUCLEAR REACTIONS 27Al, 58Ni(58Ni, X), (58Ni, F), E=14.4 MeV/nucleon; measured fusion-fission fragment σ(θ); deduced light particle evaporation mechanism in fission.

doi: 10.1007/BF01303019
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1993SZ02      Phys.Rev.Lett. 70, 2070 (1993)

A.Szanto de Toledo, E.M.Szanto, M.Wotfe, B.V.Carlson, R.Donangelo, W.Bohne, K.Grabisch, H.Morgenstern, S.Proschitzki

Are Hot Light Nuclei Liquid Droplets ( Question )

NUCLEAR REACTIONS 9Be, 10B(10B, X), E ≈ 11 MeV/nucleon; measured σ(evaporation residue, A); deduced no shell effects, composite nuclei liquid droplet behavior.

doi: 10.1103/PhysRevLett.70.2070
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1992PA24      Nucl.Instrum.Methods Phys.Res. A322, 43 (1992)

G.Pausch, W.Bohne, H.Fuchs, D.Hilscher, H.Homeyer, H.Morgenstern, A.Tutay, W.Wagner

Particle Identification in Solid-State Detectors by Exploiting Pulse Shape Information

NUCLEAR REACTIONS 197Au(32S, X), E=795 MeV; 165Ho(12C, X), E=380 MeV; measured fragment charge, energy; deduced signal processing technique features, fragment charge resolutions.

doi: 10.1016/0168-9002(92)90356-9
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1990BO01      Phys.Rev. C41, R5 (1990)

W.Bohne, H.Morgenstern, K.Grabisch, T.Nakagawa, S.Proschitzki

Critical Excitation Energy in Fusion-Evaporation Reactions

NUCLEAR REACTIONS 45Sc, 51V, 58Ni(32S, X), E=708, 955 MeV; 58Ni(32S, X), E=836 MeV; 56Fe(32S, X), E=708 MeV; calculated evaporation residue mass widths; deduced hot excited nucleus decay features.

doi: 10.1103/PhysRevC.41.R5
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1988NA11      Nucl.Instrum.Methods Phys.Res. A271, 523 (1988)

T.Nakagawa, W.Bohne

A Compact and Gridless Channel Plate Start Detector

NUCLEAR REACTIONS 58Ni(32S, X), E=710 MeV; measured evaporation residue σ(θ) vs velocity. Gridless channel plate start detector.

doi: 10.1016/0168-9002(88)90315-4
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1986MO15      Z.Phys. A324, 443 (1986)

H.Morgenstern, W.Bohne, W.Galster, K.Grabisch

Study of the Reaction Mechanism of Incomplete Fusion with the Reactions 40Ar + 11B, 12,13C at 7 MeV/amu

NUCLEAR REACTIONS 11B, 12,13C(40Ar, X), E=278 MeV; measured σ(evaporation residue θ), fragment velocity vs mass spectra; deduced incomplete fusion reaction mechanism. Evaporation code. Tof.


1984BL09      J.Phys.(Paris), Colloq.C4, 201 (1984); See 1984Bl23

Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, W.Von Oertzen, M.Buenerd, A.Gamp, D.Lebrun, Ph.Martin

High Excitation Energy Structures in Heavy Ion Collisions on a 208Pb Target


1984BL23      J.Phys.(Paris), Colloq.C-4, 201 (1984)

Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, W.von Oertzen, M.Buenerd, A.Gamp, D.Lebrun, Ph.Martin

High Excitation Energy Structures in Heavy Ion Collisions on a 208Pb Target

NUCLEAR REACTIONS 208Pb(36Ar, X), E=11 MeV/nucleon; 208Pb(20Ne, X), E=30 MeV/nucleon; measured fragment σ(θ), σ(EX, θX). Tof spectrometer.


1984CH18      Z.Phys. A318, 41 (1984)

Ph.Chomaz, N.Frascaria, Y.Blumenfeld, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, A.Gamp, W.Von Oertzen, M.Buenerd, D.Lebrun, Ph.Martin

High Excitation Energy Structures in 208Pb

NUCLEAR REACTIONS 208Pb(36Ar, 36Ar'), E=11 MeV/nucleon; 208Pb(20Ne, 20Ne'), E=30 MeV/nucleon; measured σ(θ), σ(θ, E(36Ar')), σ(θ, E(20Ne')); deduced reaction mechanism. 208Pb deduced high excitation structures, excitation process, Γ. DWBA analysis.

doi: 10.1007/BF02117213
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1984CH28      Z.Phys. A319, 167 (1984)

Ph.Chomaz, Y.Blumenfeld, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, A.Gamp, W.Von Oertzen, Nguyen Van Giai, D.Vautherin

High Energy Structures in Heavy Ion Collisions: A multi-phonon description

NUCLEAR REACTIONS 208Pb(36Ar, X), E=11 MeV/nucleon; measured σ(fragment E, θ) for 35Cl, 38Ar transfer; deduced structure, giant resonance based multiphonon excitation mechanism, role in kinetic energy dissipation.

doi: 10.1007/BF01415630
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1984LE06      Nucl.Phys. A415, 149 (1984)

H.Lehr, W.Bohne, K.Grabisch, H.Morgenstern, W.Von Oertzen

Complete Fusion in a Light Heavy-Ion Reaction from 2.5 to 20 MeV/Nucleon

NUCLEAR REACTIONS, ICPND 26Mg(20Ne, X), E=51-395 MeV; measured evaporation residues, σ vs mass, E. Statistical model calculations.

doi: 10.1016/0375-9474(84)90604-3
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1984MO02      Phys.Rev.Lett. 52, 1104 (1984)

H.Morgenstern, W.Bohne, W.Galster, K.Grabisch, A.Kyanowski

Influence of the Mass Asymmetry on the Onset of Incomplete and the Limit to Complete Fusion

NUCLEAR REACTIONS 12,13C, 26Mg, 27Al, 40,44,48Ca, 58,60,62Ni(12C, X), (20Ne, X), (22Ne, X), (35Cl, X), (36Ar, X), (40Ar, X), E=10-25 MeV/nucleon; measured σ(evaporation residue θ) vs velocity; deduced incomplete fusion onset, complete fusion limit.

doi: 10.1103/PhysRevLett.52.1104
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1983BO20      Z.Phys. A313, 19 (1983)

W.Bohne, P.Frobrich, K.Grabisch, K.Hartmann, H.Lehr, H.Morgenstern, W.Stoffler

Analysis of the Evaporation-Corrected Mass and Charge Distributions in Ar + Mo Reactions

NUCLEAR REACTIONS 100Mo(40Ar, X), 92Mo(36Ar, X), E=270 MeV; measured σ(fragment E, mass, Z), σ(fragment E, mass, Z, θ) vs total kinetic energy loss for X=26Mg, 35S, 36,37Cl, 44Ca. Surface friction model.

doi: 10.1007/BF02115839
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1983CA18      Z.Phys. A313, 57 (1983)

J.Carter, C.Brendel, A.Richter, G.Schrieder, H.Feldmeier, W.Bohne, K.Grabisch, H.Lehr, H.Morgenstern

On the Fusion Dynamics of 40Ar + 40Ca - Fussion-Fission and Fusion-Evaporation

NUCLEAR REACTIONS 40Ca(40Ar, X), E=161, 190, 236, 273 MeV; measured σ(evaporation residue θ), total σ(evaporation residue) vs mass; deduced fusion L(maximum). Trajectory model, rotational, neck degrees of freedom.

doi: 10.1007/BF02115843
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1983MO13      Z.Phys. A313, 39 (1983)

H.Morgenstern, W.Bohne, K.Grabisch, H.Lehr, W.Stoffler

Formation and Decay of the Compound Nucleus Studied in the Reaction 20Ne + 27Al

NUCLEAR REACTIONS, ICPND 27Al(20Ne, xnypzα), E=51-95; 27Al(22Ne, xnypzα), E=117 MeV; measured evaporation residue σ(E), evaporation residue velocity spectra. 27Al(20Ne, xnypzα), E=150 MeV; measured σ(evaporation residue θ); deduced α, nucleon evaporation competition.

doi: 10.1007/BF02115841
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1983OE04      Phys.Lett. 127B, 177 (1983)

H.Oeschler, M.Kollatz, W.Bohne, K.Grabisch, H.Lehr, H.Freiesleben, K.D.Hildenbrand

Complete Fusion in Peripheral Collisions Observed in the Reaction 16O on 146Nd at 10 MeV/u

NUCLEAR REACTIONS 146Nd(16O, F), (16O, X), E=161 MeV; measured fission fragment σ(θ), σ(evaporation residue θ); deduced peripheral collision complete fusion.

doi: 10.1016/0370-2693(83)90871-7
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1982BO14      Nucl.Phys. A378, 525 (1982)

W.Bohne, K.D.Buchs, H.Fuchs, K.Grabisch, D.Hilscher, U.Jahnke, H.Kluge, T.G.Masterson, H.Morgenstern

Study of the Reactions 24,26Mg(3He, n)26,28Si and 28Si(3He, n)30S

NUCLEAR REACTIONS 24,26Mg, 28Si(3He, n), E=13 MeV; measured σ(En, θ). 26,28Si, 30S deduced levels, L, J, π. Enriched targets.

doi: 10.1016/0375-9474(82)90463-8
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1982BU22      Z.Phys. A309, 183 (1982)

M.Burgel, W.Bohne, H.Fuchs, K.Grabisch, H.Homeyer, Ch.Egelhaaf

Search for Localization of ' Fast Fission ' in Angular Momentum

NUCLEAR REACTIONS 165Ho(40Ar, F), E=271 MeV; measured fission σ(fragment θ), σ(fragment) vs mass; deduced no localized fast fission.


1982MO15      Phys.Lett. 113B, 463 (1982)

H.Morgenstern, W.Bohne, K.Grabisch, D.G.Kovar, H.Lehr

Incomplete Momentum Transfer in Heavy-Ion Fusion at 14.5 MeV/Nucleon

NUCLEAR REACTIONS 12C, 27Al, 40Ca(20Ne, X)32S/47V/60Zn, E=291 MeV; measured σ (fragment θ) vs velocity; deduced incomplete momentum transfer in fusion.

doi: 10.1016/0370-2693(82)90786-9
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1979BO36      Nucl.Phys. A332, 501 (1979)

W.Bohne, K.Grabisch, J.Hergesell, Q.Liu, H.Morgenstern, W.Von Oertzen, W.Galster, W.Treu, H.H.Wolter

A Study of Two-Step Transfer Contributions to the Inelastic Scattering of 13C on 16O and 18O

NUCLEAR REACTIONS 16O(13C, 13C), (13C, 12C), 18O(13C, 12C), (13C, 13C), (13C, 14C), E=24 MeV; measured σ(θ). 17O, 19O levels deduced L, S. Enriched targets. Coupled-channel analysis.

doi: 10.1016/0375-9474(79)90015-0
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1977BO16      Nucl.Phys. A284, 14 (1977)

W.Bohne, K.D.Buchs, H.Fuchs, K.Grabisch, D.Hilscher, U.Jahnke, H.Kluge, T.G.Masterson, H.Morgenstern

The Reactions 36,38,40Ar(3He, n)38,40,42Ca and 40,42Ca(3He, n)42,44Ti

NUCLEAR REACTIONS 36,38,40Ar(3He, n), E=11.5 MeV; 40,42Ca(3He, n), E=13 MeV; measured σ(En, θ). 38,40,42Ca, 42,44Ti deduced levels, L, J, π, T. Enriched targets.

doi: 10.1016/0375-9474(77)90682-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0797.


1975BO04      Nucl.Phys. A240, 171 (1975)

W.Bohne, H.Fuchs, K.Grabisch, H.Kluge, H.Morgenstern, H.Oeschler, W.Schlegel

Observation of Weakly Coupled 2p-1h States in 41Ca from Proton Transfer on 40K

NUCLEAR REACTIONS 40K(3He, d), E=13, 21 MeV; 40K(d, n), E=6.5 MeV; measured σ(Ed, θ), σ(En, θ). 41Ca deduced levels, L, S, J, π. Enriched target.

doi: 10.1016/0375-9474(75)90443-1
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1975BO14      Nucl.Phys. A245, 107 (1975)

W.Bohne, H.Fuchs, K.Grabisch, D.Hilscher, U.Jahnke, H.Kluge, T.G.Masterson, H.Morgenstern

Nuclear Spectroscopy and Study of Pairing Modes Near N = 28 with the (τ, n) Reaction

NUCLEAR REACTIONS 48,50Ti, 50,52Cr, 54Fe(3He, n), E(3He)=13 MeV; measured σ(En, θ). 50,52Cr, 52,54Fe, 56Ni deduced levels, L, J, π, T. Enriched targets.

doi: 10.1016/0375-9474(75)90084-6
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1975GA17      Nucl.Phys. A250, 341 (1975)

A.Gamp, P.Braun-Munzinger, C.K.Gelbke, H.L.Harney, H.G.Bohlen, W.Bohne, K.D.Hildenbrand, J.Kuzminski, W.Von Oertzen, I.Tserruya

Interfering Proton and Neutron Transfer in the Reaction 13C(15N, 14N)14C

NUCLEAR REACTIONS 13C(15N, 14N)(15N, 14C), E=30, 32, 45 MeV; measured σ(θ); deduced spectroscopic amplitudes. Enriched targets.

doi: 10.1016/0375-9474(75)90264-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1692.


1975TS01      Nucl.Phys. A242, 345 (1975)

I.Tserruya, W.Bohne, P.Braun-Munzinger, C.K.Gelbke, W.Grochulski, H.L.Harney, J.Kuzminski

Transfer Reactions Induced by 16O on 29,30Si

NUCLEAR REACTIONS 28,29,30Si(16O, 16O), 29,30Si(16O, 15N), 29Si(16O, 15O), 29,30Si(16O, 17O), 30Si(16O, 14C), 30Si(16O, 18O), E(lab)=73.5 MeV; measured σ(θ). 28,29,30Si, 30,31P, 32S levels deduced S. Recoil DWBA analysis. Enriched targets.

doi: 10.1016/0375-9474(75)90054-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1779.


1974BO15      Nucl.Phys. A222, 117 (1974)

W.Bohne, C.K.Gelbke, P.Braun-Munzinger, W.Grochulski, H.L.Harney, H.Oeschler

Elastic Transfer of a 1p3/2 Hole in the Scattering of 12C on 11B

NUCLEAR REACTIONS 11B(12C, 12C), E=15, 17, 20, 24 MeV; measured σ(θ). Enriched targets.

doi: 10.1016/0375-9474(74)90587-9
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1974GA37      Nucl.Instrum.Methods 120, 281 (1974)

A.Gamp, W.Bohne, P.Braun-Munzinger, C.K.Gelbke

Complete Identification of Heavy Ions by Means of a Time-of-Flight Spectrometer with ΔE Ionization Chamber

NUCLEAR REACTIONS 12C, 16O, 30Si(16O, X), E=84 MeV; 13C(15N, X), E=32 MeV; measured mass yields.

doi: 10.1016/0029-554X(74)90047-0
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1973BO50      Phys.Lett. 47B, 342 (1973)

W.Bohne, H.Fuchs, K.Grabisch, D.Hilscher, U.Jahnke, H.Kluge, T.G.Masterson

New States in 16F

NUCLEAR REACTIONS 14N(3He, n), E=10, 12.5, 13 MeV; measured σ(En, θ). 16F deduced levels, J, π, L.

doi: 10.1016/0370-2693(73)90618-7
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1973BR25      Phys.Rev.Lett. 31, 1423 (1973)

P.Braun-Munzinger, W.Bohne, C.K.Gelbke, W.Grochulski, H.L.Harney, H.Oeschler

Strongly Oscillating Angular Distributions in the Reaction 32S(16O, 12C)36Ar at E(c.m.) = 30 MeV

NUCLEAR REACTIONS 32S(16O, 12C), (16O, 16O), E=45 MeV; measured σ(θ). 36Ar deduced transitions.

doi: 10.1103/PhysRevLett.31.1423
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1972BO49      Nucl.Phys. A196, 41 (1972)

W.Bohne, J.Bommer, H.Fuchs, K.Grabisch, H.Kluge, G.Roschert

Study of the (d, n) and (d, p) Reactions on 15N

NUCLEAR REACTIONS 15N(d, d0), (d, p), (d, n), E=4.25-6.25 MeV; measured σ(E;Ep, θ), σ(E;En, θ). 16O, 16N deduced levels, L, J, π, T, S. Enriched targets.

doi: 10.1016/0375-9474(72)90947-5
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1971BO02      Nucl.Phys. A160, 257 (1971)

W.Bohne, H.Homeyer, H.Lettau, H.Morgenstern, J.Scheer, F.Sichelschmidt

Study of States in 16O by the Reactions 17O(t, α)16O and 15N(t, d)16O

NUCLEAR REACTIONS 17O(3He, α), 15N(3He, d), E=11 MeV; measured σ(Eα, θ(α)), σ (Ed, θ(d)). 16O levels deduced L, J, S. Enriched targets.

doi: 10.1016/0375-9474(71)90130-8
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1970BO07      Phys.Rev.Lett. 24, 1028 (1970)

W.Bohne, M.Hagen, H.Homeyer, H.Lettau, K.H.Maier, H.Morgenstern, J.Scheer

Singlet Deuteron Emission in a (He3, d) Reaction Described by Distorted-Wave Born Approximation

NUCLEAR REACTIONS 10B(3He, d), 10B(3He, np), E=8, 10, 11 MeV; measured σ(θ), σ(En, Ep); deduced emission of singlet deuterons.

doi: 10.1103/PhysRevLett.24.1028
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1970BO21      Nucl.Phys. A154, 105 (1970)

W.Bohne, H.Homeyer, H.Lettau, H.Morgenstern, J.Scheer, F.Sichelschmidt

A Study of the Reaction 15N(tau, α)14N

NUCLEAR REACTIONS 15N(3He, α), E=11 MeV; measured (θ(α), Eα). 14N levels deduced L, J, S. Enriched target. 15N(3He, 3He), E=11 MeV; measured σ(θ); deduced optical parameters.

doi: 10.1016/0375-9474(70)91072-9
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1970BO25      Nucl.Phys. A156, 93 (1970)

W.Bohne, H.Homeyer, H.Lettau, H.Morgenstern, J.Scheer

Optical-Model Analysis of Elastic tau Scattering on the Nuclei with A = 15-18 at 11 MeV

NUCLEAR REACTIONS 15N, 16O, 17O, 18O(3He, 3He), E=11 MeV; measured σ(θ); deduced optical-model parameters. Enriched targets.

doi: 10.1016/0375-9474(70)91117-6
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1970BO34      Nucl.Phys. A157, 593 (1970)

W.Bohne, J.Bommer, H.Fuchs, K.Grabisch, M.Hagen, H.Homeyer, U.Janetzki, H.Lettau, H.Morgenstern, G.Roschert, J.Scheer

Transfer Reactions Leading to States of 11C

NUCLEAR REACTIONS 10B(d, n), E=5.8 MeV; 10B(3He, d), E=11.0 MeV; 12C(3He, α), E=9.5, 10.5, 11.5 MeV; measured σ(En, θ), σ(Ed, θ), σ(Eα, θ). 11C deduced L, J, π, S. Enriched 10B targets.

doi: 10.1016/0375-9474(70)90236-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0281.


1970BO39      Phys.Rev. C2, 2072 (1970)

W.Bohne, M.Hagen, H.Homeyer, K.H.Maier, H.Lettau, H.Morgenstern, J.Scheer

Study of Particle-Emitting States in N12 and C12 Formed in Reactions of B10 with Helions

NUCLEAR REACTIONS 10B(3He, n), E=6.2 MeV; 10B(3He, n), (3He, p), E=10, 11 MeV; measured σ(En, θ), σ(Ep, θ), σ(En, Ep, θ(np)), σ(Ep1, Ep2, θ(pp)), σ(Ep, Eα, θ(pα)). 12N, 12C deduced levels, particle branching ratios.

doi: 10.1103/PhysRevC.2.2072
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1969BO13      Nucl.Phys. A128, 537 (1969)

W.Bohne, H.Homeyer, H.Lettau, H.Morgenstern, J.Scheer, F.Sichelschmidt

Study of States in 16O by the Reaction 15N(3He, d)16O

NUCLEAR REACTIONS 15N(3He, d), E=11 MeV; measured σ(θ(d), Ed). 16O levels deduced L, S. Enriched target. 15N(3He, t), E=11 MeV; measured σ(θ(t)).

doi: 10.1016/0375-9474(69)90421-7
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1969BO18      Nucl.Phys. A131, 273 (1969)

W.Bohne, H.Fuchs, K.Grabisch, M.Hagen, H.Homeyer, U.Janetzki, H.Lettau, K.H.Maier, H.Morgenstern, P.Pietrzyk, G.Roschert, J.A.Scheer

One-Proton and Two-Proton Stripping Between 26Mg, 27Al and 28Si

NUCLEAR REACTIONS 26Mg(3He, n), E=5.7 MeV; 26Mg(3He, d), 26Mg(3He, α), E=11 MeV; 27Al(d, n), E=6 MeV; measured σ(E, θ). 25Mg, 27Al, 28Si deduced levels, L, π, S, T. Enriched targets.

doi: 10.1016/0375-9474(69)90537-5
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1968BO02      Nucl.Phys. A106, 442 (1968)

W.Bohne, D.Hilscher, H.Homeyer, H.Morgenstern, J.A.Scheer

Neutron-Proton Correlations in the Reaction 12C(d, np)12C

NUCLEAR REACTIONS 12C(d, np)12C; E = 5.4, 6.0 MeV, measured σ(Ep, En, θ(np)); deduced reaction modes. Natural target.

doi: 10.1016/0375-9474(67)90888-3
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1968BO08      Nucl.Phys. A111, 417(1968)

W.Bohne, D.Hilscher, H.Homeyer, H.Morgenstern, J.A.Scheer

Neutron-Induced Reactions on Silicon. Deuteron and Alpha Particle Angular Distributions at E = 21.3 MeV

NUCLEAR REACTIONS 28Si(n, d), (n, α), E=14-22 MeV; measured σ(E;Eα, θ). 27Al deduced levels, S. Natural target.

doi: 10.1016/0375-9474(68)90134-6
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1968BO14      Nucl.Phys. A113, 97(1968)

W.Bohne, H.Homeyer, H.Morgenstern, J.Scheer

Study of States in 15O by the Reactions 14N(3He, d) and 16O(3He, α)

NUCLEAR REACTIONS 14N(3He, d), 16O(3He, α), E=11 MeV; measured σ(delta). 15O deduced levels, S. Natural targets.

doi: 10.1016/0375-9474(68)90886-5
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1968BO26      Nucl.Phys. A115, 457(1968)

W.Bohne, H.Homeyer, H.Morgenstern, J.Scheer

Study of States in 12C by the Reaction 11B(t, d)12C

NUCLEAR REACTIONS 11B(3He, d), E = 11 MeV; measured σ(Ed, θ). 12C levels deduced S. Enriched target.

doi: 10.1016/0375-9474(68)90018-3
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