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NSR database version of April 27, 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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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