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NSR database version of May 23, 2024.

Search: Author = H.Bohn

Found 27 matches.

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1992CZ01      Nucl.Phys. A542, 278 (1992)

J.Czakanski, W.Zipper, M.Siemaszko, W.Dunnweber, W.Hering, D.Konnerth, W.Trombik, K.G.Bernhardt, H.Bohn, K.A.Eberhard, R.Vandenbosch

Critical Angular Momentum of Cluster Evaporation: 16O(16O, α)28Si and 16O(16O, 8Be)24Mg

NUCLEAR REACTIONS 16O(16O, α), (16O, 8Be), E(cm)=18.35-31.0 MeV; measured σ(θ) vs E; deduced angular momentum limitation for cluster emission. Hauser-Feshbach model calculations with potential-barrier penetration coefficients.

doi: 10.1016/0375-9474(92)90217-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1257.


1989KU04      Phys.Lett. 218B, 421 (1989)

R.Kulessa, R.Bengtsson, H.Bohn, H.Emling, T.Faestermann, F.von Feilitzsch, E.Grosse, W.Nazarewicz, D.Schwalm, H.J.Wollersheim

Angular Momentum Dependence of the Quadrupole Deformation in 182,184,186W

NUCLEAR REACTIONS 182,184,186W(208Pb, 208Pb'), E=4.9 MeV/nucleon; measured Doppler shifted γ-spectra following Coulomb excitation. 182,184,186W deduced yrast level B(λ), quadrupole moments.

doi: 10.1016/0370-2693(89)91439-1
Citations: PlumX Metrics


1987CZ02      Phys.Lett. 199B, 166 (1987)

J.Czakanski, W.Zipper, W.Dunnweber, W.Hering, D.Konnerth, W.Trombik, K.G.Bernhardt, H.Bohn, K.A.Eberhard, R.Vandenbosch

Angular Momentum Limitation of Cluster Emission from the Compound Nucleus: 16O(16O, α)28Si and 16O(16O, 8Be)24Mg

NUCLEAR REACTIONS, MECPD 16O(16O, α), (16O, 8Be), E=36-62 MeV; measured σ(θ) vs E. Si detectors. Hauser-Feshbach model.

doi: 10.1016/0370-2693(87)91352-9
Citations: PlumX Metrics


1984AR21      At.Energ. 57, 249 (1984); Sov.At.Energy 57, 702 (1984)

R.Arlt, H.Bohn, W.Wagner, M.Josch, G.Musiol, H.-G.Ortlepp, G.Pausch, K.Herbach, I.D.Alkhazov, E.A.Ganza, L.V.Drapchinsky, V.N.Dushin, S.S.Kovalenko, O.I.Kostochkin, V.N.Kuzmin, K.A.Petrzhak, B.V.Rumyantsev, S.M.Soloviev, P.S.Soloshenkov, A.V.Fomichev, V.I.Shpakov

Absolute Measurements of the 239Pu Fission Cross Section for 8.5-MeV Neutrons

NUCLEAR REACTIONS 239Pu(n, F), E=8.5 MeV; measured absolute fission σ.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30706.


1984GE03      Phys.Rev. C29, 1684 (1984)

J.Gerl, Th.W.Elze, H.Ower, H.Bohn, T.Faestermann, N.Kaffrell, N.Trautmann

Electromagnetic Properties of 230Th Studied by Coulomb Excitation

NUCLEAR REACTIONS 230Th(32S, 32S'γ), E=135 MeV; measured Coulomb excitation, Eγ, Iγ(θ(p)). 230Th deduced levels J, π, K, electromagnetic matrix elements, γ-branching, interband, intrabrand B(E2), B(E1), band structure.

doi: 10.1103/PhysRevC.29.1684
Citations: PlumX Metrics


1983GE01      Phys.Lett. 120B, 83 (1983)

J.Gerl, Th.W.Elze, H.Ower, K.Ronge, H.Bohn, T.Faestermann

Rotation-Vibration Interaction Strength in 232Th

NUCLEAR REACTIONS 232Th(32S, 32S'), E=135 MeV; measured Coulomb excitation, γ(32S)-coin. 232Th deduced γ-branching, B(E2) ratio. Collective model.

doi: 10.1016/0370-2693(83)90628-7
Citations: PlumX Metrics


1981BE29      Nucl.Phys. A365, 157 (1981)

K.G.Bernhardt, H.Bohn, K.A.Eberhard, R.Sielemann, R.Vandenbosch, M.P.Webb

The 12C(18O, α)26Mg and 12C(18O, 8Be)22Ne Reaction

NUCLEAR REACTIONS 12C(18O, 8Be), (18O, α), E(cm)=15-22.4 MeV; measured σ(E, θ); deduced no correlated structure. Statistical model calculations.

doi: 10.1016/0375-9474(81)90393-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0487.


1981BE64      Fizika(Zagreb) 13, Suppl.No.1, 27 (1981)

C.Beck, R.M.Freeman, F.Haas, B.Heusch, H.Bohn, K.A.Eberhard, U.Kaufl, H.Puchta, T.Senftleben, W.Trautmann

Resonant Structure in the Reaction Channels of 14C + 14C

NUCLEAR REACTIONS 14C(14C, 14C'), (14C, xn), (14C, xnα), E(cm)=12.5-32.5 MeV; measured σ(E), production σ(E) for 25Mg, 22Ne, Ne, 15C; deduced channel correlated structure. 28Mg deduced possible quasimolecular resonances.


1981BO29      Z.Phys. A302, 51 (1981)

H.Bohn, E.Endres, T.Faestermann, P.Kienle

Spectroscopy of Excited States in 212Po, 210Pb, and 213At Empolying 18O Induced Few-Nucleon Transfer Reactions

NUCLEAR REACTIONS 208Pb(18O, 14C), (18O, 16O), (18O, 15N), E=75, 78, 80 MeV; 209Bi(18O, 14C), (18O, 15N), E=79 MeV; measured Eα, Iα, Eγ, Iγ, γγ-, γ(18O)-, γα-coin, γ(t). 212Po, 210Pb deduced levels, yrast isomer J, π, T1/2, B(E2). 213At deduced levels.

doi: 10.1007/BF01425102
Citations: PlumX Metrics


1981DA08      Z.Phys. A300, 71 (1981)

G.Dannhauser, J.de Boer, R.Lutter, F.Riess, H.Bohn

The Quadrupole Moment Q2+ of 32S

NUCLEAR REACTIONS 60Ni(32S, 32S'), E=70-73 MeV; measured 32Sγ-coin, Coulomb excitation. 32S level deduced quadrupole moment.


1981FR23      Phys.Rev. C24, 2390 (1981)

R.M.Freeman, C.Beck, F.Haas, B.Heusch, H.Bohn, U.Kaufl, K.A.Eberhard, H.Puchta, T.Senftleben, W.Trautmann

Structure in the Reaction Channels of 14C + 14C

NUCLEAR REACTIONS 14C(14C, 14C'), (14C, X), E(cm)=12.5-32.5 MeV; measured Eγ, Iγ; deduced production σ(E) for 15C, 21,22,23Ne, 25Mg, channel correlated resonance structure. Enriched target.

doi: 10.1103/PhysRevC.24.2390
Citations: PlumX Metrics


1981GI14      Nucl.Instrum.Methods 188, 535 (1981)

G.Giorginis, H.Bohn, T.Faestermann, F.V.Feilitzsch, P.Kienle, C.Kozhuharov, T.Yamazaki

The Electrostatic Ellipsoidal Mirror: A fast and efficient separator for slowly recoiling and highly charged nuclei

RADIOACTIVITY 212At [from 209B(α, n), E=22 MeV]; 212Po [from 209Bi(α, p), E=33 MeV]; measured Eα, Iα(t). Electrostatic ellipsoidal mirror.

doi: 10.1016/0029-554X(81)90264-0
Citations: PlumX Metrics


1981KO30      Phys.Rev. C24, 2076 (1981)

I.Koenig, H.Bohn, T.Faestermann, P.Kienle, H.J.Korner, W.A.Mayer, D.Pereira, K.E.Rehm, H.J.Scheerer

Spectroscopy of Excited States in 102Mo and 106Ru

NUCLEAR REACTIONS 100Mo(18O, 16O), E=84 MeV; 104Ru(18O, 16O), E=84, 100 MeV; measured 16Oγ-coin, Eγ. 102Mo, 106Ru deduced levels, J, π, yrast transitions. Enriched targets.

doi: 10.1103/PhysRevC.24.2076
Citations: PlumX Metrics


1980BO37      Verh.Deut.Phys.Ges. 15, 1231 G9.1 (1980)

H.Bohn, E.Endres, T.Faestermann, P.Kienle

Investigation of nuclei with N > 126 near 208Pb


1979CH07      Phys.Rev.Lett. 42, 687 (1979)

Y.-d.Chan, H.Bohn, R.Vandenbosch, R.Sielemann, J.G.Cramer, K.G.Bernhardt, H.C.Bhang, D.T.C.Chiang

Influence of Extra Neutrons Added to the 12C + 16O System: Gross Structures in γ-Ray Yields Following the 13C + 16O and 12C + 18O Reactions

NUCLEAR REACTIONS 13C(16O, Xγ), 12C(18O, Xγ), E(cm)=7-25 MeV; measured σ(E, Eγ), Iγ. Compared structures in α-decay channels.

doi: 10.1103/PhysRevLett.42.687
Citations: PlumX Metrics


1979EB01      Phys.Rev.Lett. 42, 432 (1979)

K.A.Eberhard, H.Bohn, K.G.Bernhardt

Narrow Iπ = 10+ Resonance for 12C + 16O in the Region of Strong Absorption

NUCLEAR REACTIONS 12C(16O, 8Be), E(cm)=18.8 MeV; measured σ(θ). 28Si deduced resonance, J, π, Γ.

doi: 10.1103/PhysRevLett.42.432
Citations: PlumX Metrics


1979ES04      Phys.Rev. C19, 2224 (1979)

H.Essel, K.E.Rehm, H.Bohn, H.J.Korner, H.Spieler

Inelastic Scattering of 18O and 17O Ions from Medium-Weight Nuclei

NUCLEAR REACTIONS 48Ti(18O, 18O), (18O, 18O'), E=54 MeV; 52Cr(18O, 18O), (18O, 18O'), E=56 MeV; 54Fe(18O, 18O), (18O, 18O'), E=60 MeV; 72Ge, 91Zr(18O, 18O), (18O, 18O'), E=68.6 MeV; 92Zr(18O, 18O), (18O, 18O'), E=68.5 MeV; 54Fe(17O, 17O), (17O, 17O'), E=59.1 MeV; 60Ni(17O, 17O), (17O, 17O'), E=62.1 MeV; 54Fe(18O, 17O), E=56 MeV; 120Sn(18O, 17O), E=72 MeV; 54Fe(17O, 16O), E=59.1 MeV; 60Ni(17O, 16O), E=62.1 MeV; measured σ(θ). 72Ge(18O, 18O'), E=30-48 MeV; measured σ(E). 48Ti, 52Cr, 54Fe, 60Ni, 72Ge, 91,92Zr, 17,18O levels deduced deformation lengths, B(E2). Optical, DWBA models. Enriched targets.

doi: 10.1103/PhysRevC.19.2224
Citations: PlumX Metrics


1979FA01      Phys.Lett. 80B, 190 (1979)

T.Faestermann, H.Bohn, F.v.Feilitzsch, A.W.Sunyar, R.Broda, P.Kleinheinz, M.Ogawa

Shell Model Isomers Near Z = 64, N = 82: g-Factors of Yrast States in 146Gd and 147Gd

NUCLEAR MOMENTS 146mGd, 147mGd [from 122,124Sn(28Si, X), E=119, 132 MeV]; measured γ(θ, H, t); deduced nuclear g-factors. Compared with shell model.

doi: 10.1016/0370-2693(79)90195-3
Citations: PlumX Metrics


1978CH15      Nucl.Phys. A303, 500 (1978)

Y.-D.Chan, H.Bohn, R.Vandenbosch, K.G.Bernhardt, J.G.Cramer, R.Sielemann, L.Green

Gross Structure in γ-Ray Yields Following the 16O + 12C Reaction

NUCLEAR REACTIONS 12C(16O, X), E=15-72 MeV; measured Iγ; deduced σ(E). Isotopic target.

doi: 10.1016/0375-9474(78)90373-1
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1977BO21      Phys.Rev. C16, 665 (1977)

H.Bohn, K.A.Eberhard, R.Vandenbosch, K.G.Bernhardt, R.Bangert, Y-d.Chan

Back-Angle Anomalies in 6Li Scattering from 40Ca and 44Ca

NUCLEAR REACTIONS 40,44Ca(6Li, 6Li), (6Li, 6Li'), E=30 MeV; measured σ(θ). Optical model, coupled channel, Hauser-Feshbach calculations.

doi: 10.1103/PhysRevC.16.665
Citations: PlumX Metrics


1976HE14      Phys.Rev. C14, 1451 (1976)

W.R.Hering, H.Puchta, W.Trautmann, R.L.McGrath, H.Bohn

Observation of Excited States in 206Hg

NUCLEAR REACTIONS 204Hg(18O, 16O), E=75 MeV; 204Hg(17O, 16O), E=81 MeV; measured particle-γ, γγ-coin. 206Hg deduced levels, J. Enriched targets.

doi: 10.1103/PhysRevC.14.1451
Citations: PlumX Metrics


1975BO39      Z.Phys. A274, 327 (1975)

H.Bohn, P.Kienle, D.Proetel, R.L.Hershberger

Structure of Excited States in 100Mo and 102Mo from Spectroscopy Using 18O Induced Reactions

NUCLEAR REACTIONS 100Mo(18O, 18O'γ), (18O, 16O), E=40 MeV; measured recoil distance DSA. 100,102Mo levels deduced T1/2, β, B(λ).

doi: 10.1007/BF01434042
Citations: PlumX Metrics


1974HA48      Phys.Lett. 52B, 329 (1974)

O.Hausser, D.J.Donahue, R.L.Hershberger, R.Lutter, F.Riess, H.Bohn, T.Faestermann, F.V.Feilitzsch, K.E.G.Lobner

Particle-Vibration Coupling in 107Cd

NUCLEAR REACTIONS 105Pd(α, 2nγ), E=24 MeV; measured Eγ, γγ(θ, H, t). 94Zr(16O, 3nγ), E=56 MeV; measured recoil distance, γγ(θ, H, t), DSA. 107Cd levels deduced g, T1/2.

doi: 10.1016/0370-2693(74)90054-9
Citations: PlumX Metrics


1974LU03      Nucl.Phys. A229, 230 (1974)

R.Lutter, O.Hausser, D.J.Donahue, R.L.Hershberger, F.Riess, H.Bohn, T.Faestermann, F.V.Feilitzsch, K.E.G.Lobner

Negative-Parity States in Pb Isotopes: g-Factor of the 480 ns, Jπ = 9- Isomer in 200Pb

NUCLEAR REACTIONS 198,200,202Hg(α, 2nγ), E=27 MeV; measured Iγ(θ, H, t). 200,202Pb deduced g, T1/2. 204Pb level deduced g. Enriched targets.

doi: 10.1016/0375-9474(74)90785-4
Citations: PlumX Metrics


1972BO43      Phys.Rev.Lett. 29, 1337 (1972)

H.Bohn, G.Daniel, M.R.Maier, P.Kienle, J.G.Cramer, D.Proetel

Four-Nucleon Transfer from 16O to 90Zr Near the Coulomb Barrier

NUCLEAR REACTIONS 90Zr(16O, 12C), (16O, 16O'γ), E=44-58 MeV; measured σ(E), Eγ, Iγ, (16O)(γ)-delay, (12C)(γ)-coin. 94Mo deduced levels.

doi: 10.1103/PhysRevLett.29.1337
Citations: PlumX Metrics


1970BO11      Phys.Lett. 32B, 346 (1970)

H.Bohn, G.Kaindl, D.Kucheida, F.E.Wagner, P.Kienle

Change of the Nuclear Charge Radius of 189Os from Mossbauer Isomer Shifts

NUCLEAR REACTIONS 189Os(γ, γ), E=36.2, 69.6 keV; measured Mossbauer effect; deduced isomer shifts. 189Os deduced nuclear charge radius.

doi: 10.1016/0370-2693(70)90491-0
Citations: PlumX Metrics


1969WA02      Phys.Letters 28B, 548(1969)

F.Wagner, G.Kaindl, H.Bohn, U.Biebl, H.Schaller, P.Kienle

Lifetime and Magnetic Moment of the 36.2 keV Level of 189Os

NUCLEAR REACTIONS 189Os(γ, γ), E=36.2 keV; measured Mossbauer effect. 189Os level deduced T1/2.

NUCLEAR MOMENTS 189Os; measured g; deduced μ. Detector - Si(Li).

doi: 10.1016/0370-2693(69)90052-5
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