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NSR database version of May 24, 2024.

Search: Author = H.Homeyer

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2000KO38      Acta Phys.Pol. B31, 1811 (2000)

E.Kozik, A.Budzanowski, J.Galin, D.Hilscher, H.Homeyer, U.Jahnke

Fragment Heating in 40Ar + 159Tb Collisions at 9.5 MeV/Nucleon

NUCLEAR REACTIONS 159Tb(40Ar, X), E=9.5 MeV/nucleon; measured neutron multiplicity, projectile-like fragments charge, energy distributions; deduced target-like fragments excitation energy. Statistical model calculations, equal temperature hypothesis.

1999KO15      Acta Phys.Pol. B30, 139 (1999)

E.Kozik, J.Blocki, A.Budzanowski, J.Galin, D.Hilscher, H.Homeyer, U.Jahnke, T.Kozik, Z.Sosin

Correlation between Reaction Mechanism, Kinetic Energy Release and Neutron Emission in 40Ar + 159Tb Collision at 9.5 MeV/Nucleon

NUCLEAR REACTIONS 159Tb(40Ar, nX), E=9.5 MeV/nucleon; measured projectile-like fragment energy vs neutron multiplicity. Comparison with random walk model predictions.

1996KO56      Acta Phys.Pol. B27, 2241 (1996)

E.Kozik, J.Blocki, A.Budzanowski, J.Galin, D.Hilscher, H.Homeyer, U.Jahnke, T.Kozik, Z.Sosin

Charge Distribution in 40Ar + 159Tb Reaction at 9.5 MeV/nucleon

NUCLEAR REACTIONS 159Tb(40Ar, X), E=9.5 MeV/nucleon; measured projectilelike fragment σ(θ, E), neutron multiplicity, kinetic energy plots, charge distribution. Models based on random walk phenomena, one-body dissipative processes.

1995SI09      Z.Phys. A350, 327 (1995)

A.Siwek, A.Sourell, A.Budzanowski, H.Fuchs, H.Homeyer, G.Pausch, W.Kantor, G.Roschert, C.Schwarz, W.Terlau, A.Tutay

Multifragmentation Study on 30 AMeV 32S + 58Ni

NUCLEAR REACTIONS 58Ni(32S, X), E=840, 960 MeV; measured (fragment)(fragment)-coin; deduced evaporation, fission, multi-fragmentation evidence.

doi: 10.1007/BF01291190
Citations: PlumX Metrics

1995TU02      Acta Phys.Pol. B26, 1413 (1995)

A.Tutay, A.Budzanowski, H.Fuchs, H.Homeyer, G.Pausch, C.Schwarz, A.Siwek, A.Taymaz

Temporal and Thermal Properties of Intermediate-Mass Fragments from the 32S + 58Ni Reaction at 30A MeV

NUCLEAR REACTIONS 58Ni(32S, X), E=960 MeV; measured intermediate mass (fragment)(fragment)(θ), α(fragment)(θ); deduced intermediate-mass fragment thermal, temporal aspects.

1994SI14      Acta Phys.Pol. B25, 765 (1994)

A.Siwek, A.Budzanowski, H.Fuchs, H.Homeyer, W.Kantor, G.Pausch, G.Roeschert, C.Schwarz, A.Sourell, W.Terlau, A.Tutay

Multifragmentation in the Reaction 32S + 58Ni at 30 AMeV

NUCLEAR REACTIONS 58Ni(32S, X), E=30 MeV/nucleon; measured (fragment)(fragment)(fragment)-coin; deduced mass, velocity distributions, fragmentation mechanism.

1993SC10      Z.Phys. A345, 29 (1993)

C.Schwarz, H.Fuchs, H.Homeyer, K.Mohring, T.Schmidt, A.Siwek, A.Sourell, W.Terlau, A.Budzanowski

Projectile Break-Up with Two Outgoing Intermediate-Mass Fragments in 26 AMeV 32S + 197Au

NUCLEAR REACTIONS 197Au(32S, X), E=840 MeV; measured intermediate mass (fragment)(fragment)(θ); deduced fragment pair production mechanism.

doi: 10.1007/BF01290336
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
Citations: PlumX Metrics

1992SC06      Phys.Lett. 279B, 223 (1992)

C.Schwarz, H.Fuchs, H.Homeyer, K.Mohring, T.Schmidt, A.Siwek, A.Sourell, W.Terlau, A.Budzanowski

Non-Thermal Projectile Breakup Due to Friction Forces

NUCLEAR REACTIONS 197Au(32S, X), E=26 MeV/nucleon; measured σ(θα, fragment θ); deduced projectile breakup mechanism.

doi: 10.1016/0370-2693(92)90383-F
Citations: PlumX Metrics

1989AL10      Z.Phys. A333, 319 (1989)

D.Alber, O.Boebel, C.Schwarz, H.Duwe, D.Hilscher, H.Homeyer, U.Jahnke, B.Spellmeyer

Search for Neutrons from ' Cold Nuclear Fusion '

NUCLEAR REACTIONS 2H(d, n), E=low; measured no cold fusion neutrons. Deuterium loaded Pd electrode, electrolysis setup.

1988MO05      Phys.Lett. 203B, 210 (1988)

K.Mohring, T.Srokowski, D.H.E.Gross, H.Homeyer

A Dynamical Model for Projectile Break-Up and Incomplete Fusion

NUCLEAR REACTIONS 197Au, 20Ne(20Ne, X), E ≈ 100-400 MeV; measured fusion σ(E), σ(θ(X), θα). Dynamical model. Projectile breakup.

doi: 10.1016/0370-2693(88)90540-0
Citations: PlumX Metrics

1988RI01      Phys.Lett. 200B, 8 (1988)

R.Ritzka, W.Dunnweber, A.Glaesner, W.Hering, W.Trombik, A.Budzanowski, M.Burgel, H.Homeyer

Symmetry Axes of Heavy-Ion Spin Transfer from γ-Ray In-Plane Anisotropies

NUCLEAR REACTIONS 168Er(20Ne, X), E=270 MeV; measured in-plane γ-ray anisotropies, (particle)γ-coin; deduced heavy-ion spin transfer symmetry axes.

doi: 10.1016/0370-2693(88)91099-4
Citations: PlumX Metrics

1988TE03      Z.Phys. A330, 303 (1988)

W.Terlau, M.Burgel, A.Budzanowski, H.Fuchs, H.Homeyer, G.Roschert, J.Uckert, R.Vogel

Incomplete Deep-Inelastic Scattering in 20Ne + 197Au Collisions at 20 MeV/Nucleon

NUCLEAR REACTIONS 197Au(20Ne, X), E=390 MeV; measured (fragment)(fragment)-coin, σ(θα, fragment θ); deduced reaction mechanism.

1988UC01      Phys.Lett. 206B, 190 (1988)

J.Uckert, A.Budzanowski, M.Burgel, H.Fuchs, H.Homeyer, W.Terlau

The Relative Importance of Projectile Remnants and Hot Sources in Light-Particle Correlations

NUCLEAR REACTIONS 197Au(20Ne, X), E=20 MeV/nucleon; measured σ(fragment θ1, θ2), αα-coin; deduced intermediate source 8Be production σ(θ).

doi: 10.1016/0370-2693(88)91490-6
Citations: PlumX Metrics

1987BU07      Phys.Rev. C36, 90 (1987)

M.Burgel, H.Fuchs, H.Homeyer, G.Ingold, U.Jahnke, G.Thoma

Projectile-Like Fragments from 20Ne + 197Au and the Correlated Energy Transfer Studied by Counting the Simultaneously Emitted Neutrons

NUCLEAR REACTIONS 197Au(20Ne, xnX), E=290 MeV; measured projectile-like(fragment)n-coin vs neutron number, θ; deduced target excitation, fragment energy correlation, optimum Q-value, transfer, break-up distinction.

doi: 10.1103/PhysRevC.36.90
Citations: PlumX Metrics

1985FU02      Phys.Rev. C31, 465 (1985)

H.Fuchs, M.Burgel, H.Homeyer, G.Ingold, U.Jahnke, G.Thoma

Production of Fast α Particles in 20Ne + 197Au Collisions Studied by Counting the Simultaneously Emitted Neutrons

NUCLEAR REACTIONS 197Au(20Ne, xnα), E=220, 290, 400 MeV; measured σ(Eα, θα) vs neutron multiplicity; deduced relative breakup, nonequilibrium α-emission σ.

doi: 10.1103/PhysRevC.31.465
Citations: PlumX Metrics

1985WA22      Phys.Rev. C32, 894 (1985)

S.Wald, S.B.Gazes, C.R.Albiston, Y.Chan, B.G.Harvey, M.J.Murphy, I.Tserruya, R.G.Stokstad, P.J.Countryman, K.Van Bibber, H.Homeyer

Transfer and Breakup Processes in Reactions of 11- and 17-MeV/nucleon 20Ne + 197Au

NUCLEAR REACTIONS 197Au(20Ne, X), E=220, 341 MeV; measured σ(fragment E, θ, Z) for X=Li, Be, B, C, N, O, F; deduced transfer, breakup, primary ejectile yields. Coincidence techniques.

doi: 10.1103/PhysRevC.32.894
Citations: PlumX Metrics

1984HO23      Z.Phys. A319, 143 (1984)

H.Homeyer, M.Burgel, Ch.Egelhaaf, H.Fuchs, G.Thoma

Features of Direct Cluster Stripping in Primary Fragments from Quasielastic 20Ne-Induced Reactions

NUCLEAR REACTIONS 197Au(20Ne, X)20F/19F/18F/17F/19O/18O/17O/16O/15O/16N/15N/14N/15C/14C/13C/12C/12B/11B/10B, E=150, 220, 250, 400 MeV; calculated residuals yield, σ; deduced reaction mechanism. Cluster stripping model.

doi: 10.1007/BF01415626
Citations: PlumX Metrics

1983EG02      Nucl.Phys. A405, 397 (1983)

Ch.Egelhaaf, M.Burgel, H.Fuchs, A.Gamp, H.Homeyer, D.Kovar, W.Rauch

Mechanism of Neon-Induced Reactions Studied between 7.5 and 20 MeV/Nucleon: Inclusive cross sections

NUCLEAR REACTIONS 197Au(20Ne, X), (20Ne, αX), (20Ne, F), (20Ne, 20Ne), E=150, 220, 240, 400 MeV; measured σ(fragment θ, Z, mass, energy), σ(elastic), fission σ; deduced reaction mechanism. Natural target.

doi: 10.1016/0375-9474(83)90579-1
Citations: PlumX Metrics

1983HO25      Z.Phys. A314, 143 (1983)

H.Homeyer, U.Jahnke, G.Ingold, M.Burgel, H.Fuchs, D.Hilscher

Two Different Sources of Fast Forward-Emitted α-Particles in Heavy-Ion Reactions

NUCLEAR REACTIONS 197Au(20Ne, αX), E=290 MeV; analyzed σ(Eα), αn-coin multiplicity distribution; deduced α-emission mechanisms, inelasticity dependences.

doi: 10.1007/BF01879872
Citations: PlumX Metrics

1983JA05      Phys.Rev.Lett. 50, 1246 (1983)

U.Jahnke, G.Ingold, H.Homeyer, M.Burgel, Ch.Egelhaaf, H.Fuchs, D.Hilscher

Neutron Multiplicity Distributions and the Role of Transfer and Breakup in Quasielastic Heavy-Ion Reactions at 15 MeV/Nucleon

NUCLEAR REACTIONS 197Au(20Ne, X), E=15 MeV/nucleon; measured σ(fragment E) for X=19Ne, 19F, 16O, 15N, 12C, neutron multiplicities; deduced reaction mechanism. Coincidence techniques, 4π neutron multiplicity counter.

doi: 10.1103/PhysRevLett.50.1246
Citations: PlumX Metrics

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.

1982GA23      Z.Phys. A309, 49 (1982)

A.Gamp, M.Burgel, M.R.Clover, Ch.Egelhaaf, H.Fuchs, B.Gebauer, H.Homeyer, W.Rauch, J.C.Jacmart

Fast Emission of α-Particles in Deep-Inelastic 36Ar + 197Au Collisions

NUCLEAR REACTIONS 197Au(40Ar, αX), E=380 MeV; measured σ(fragment θ, θα); deduced reaction mechanism.

doi: 10.1007/BF01420150
Citations: PlumX Metrics

1982HO10      Phys.Rev. C26, 1335 (1982)

H.Homeyer, M.Burgel, M.Clover, Ch.Egelhaaf, H.Fuchs, A.Gamp, D.Kovar, W.Rauch

Dissociation of 15-MeV/Nucleon 20Ne in Collisions with 197Au: Direct reactions leading to particle-emitting states

NUCLEAR REACTIONS 197Au(20Ne, α15N), (20Ne, α16O), E=290 MeV; measured α(15N)-, α(16O)-coin; deduced quasielastic projectile dissociation.

doi: 10.1103/PhysRevC.26.1335
Citations: PlumX Metrics

1981EG01      Phys.Rev.Lett. 46, 813 (1981)

Ch.Egelhaaf, G.Bohlen, H.Fuchs, A.Gamp, H.Homeyer, H.Kluge

Small Momentum Widths in Heavy-Ion Fragmentation at 20 MeV/amu and below

NUCLEAR REACTIONS 197Au(20Ne, 16O), (20Ne, 12C), E=20 MeV/nucleon; measured σ(E(16O)), σ(E(12C)); deduced quasielastic peak momentum distribution width, no rapid change of reaction mechanism.

doi: 10.1103/PhysRevLett.46.813
Citations: PlumX Metrics

1981EG02      Phys.Rev. C24, 759 (1981)

Ch.Egelhaaf, H.Fuchs, A.Gamp, H.Homeyer

Distinction of the Deep-Inelastic and Quasi-Elastic Component in a Reaction Induced by a Light Heavy Ion

NUCLEAR REACTIONS 197Au(20Ne, 14N), (20Ne, 16O), E=400 MeV; measured σ(θ, E(14N)), σ(θ, E(16O)); deduced distinguishable deep-inelastic, quasielastic components. Natural target, ΔE-E solid state detectors.

doi: 10.1103/PhysRevC.24.759
Citations: PlumX Metrics

1981GA19      Z.Phys. A300, 63 (1981)

A.Gamp, M.Burgel, M.R.Clover, C.Egelhaaf, H.Fuchs, B.Gebauer, H.Homeyer, J.C.Jacmart

Light Particle Emission in Quasi-Elastic Heavy-Ion Reactions

NUCLEAR REACTIONS 197Au(36Ar, αX), E=380 MeV; measured αX(θ), (fragment)α energy correlation; deduced reaction mechanism. Quasielastic heavy ion reaction.

doi: 10.1007/BF01412615
Citations: PlumX Metrics

1980VO08      Z.Phys. A298, 207 (1980)

W.von Oertzen, H.Fuchs, A.Gamp, H.Homeyer, U.Jahnke, J.C.Jacmart

Evaporation Residue Cross Sections from the Fusion of 52Cr + 110Pd

NUCLEAR REACTIONS 110Pd(52Cr, X), E=211.8-240.5 MeV; measured σ(θ, E) for evaporation residues; deduced σ(reaction). 162Yb deduced level density, fission barrier parameters. Statistical evaporation calculations.

1978PI09      Phys.Rev. C18, 180 (1978)

S.C.Pieper, M.H.Macfarlane, D.H.Gloeckner, D.G.Kovar, F.D.Becchetti, B.G.Harvey, D.L.Hendrie, H.Homeyer, J.Mahoney, F.Puhlhofer, W.von Oertzen, M.S.Zisman

Energy Dependence of Elastic Scattering and One-Nucleon Transfer Reactions Induced by 16O on 208Pb. I

NUCLEAR REACTIONS 208Pb(16O, 16O), E=80-216.6 MeV; 208Pb(16O, 15N), (16O, 17O), E=104, 138.5, 216.6 MeV; measured σ(θ). Optical model, DWBA analysis.

doi: 10.1103/PhysRevC.18.180
Citations: PlumX Metrics

1976BR28      Phys.Rev. C14, 896 (1976)

D.R.Brown, I.Halpern, J.R.Calarco, P.A.Russo, D.L.Hendrie, H.Homeyer

Neutron Pickup by Alpha Particles to Unbound States

NUCLEAR REACTIONS 12C, Rh, 208Pb, U(α, 5He), E=42, 90 MeV; measured αn-coin, σ.

doi: 10.1103/PhysRevC.14.896
Citations: PlumX Metrics

1976JA14      Nucl.Phys. A267, 285 (1976)

U.Janetzki, Q.K.K.Liu, D.Hahn, H.Homeyer, J.Scheer

Normalization of the (3He, d(s)) Reaction and Nuclear Spectroscopy with the Single Doublet

NUCLEAR REACTIONS 13C(3He, d), (3He, np), E=13 MeV; measured σ(Ed, θ), σ(Ep, En, θ), E(pn)=0; deduced singlet deuteron, optical model parameters, normalization constants. 11C, 14N levels deduced S. Enriched target.

doi: 10.1016/0375-9474(76)90661-8
Citations: PlumX Metrics

1976VO07      Z.Phys. A279, 357 (1976)

W.von Oertzen, H.Homeyer, B.G.Harvey, D.Hendrie, D.Kovar

Two Proton Transfer Reactions between Pairing Rotational States with 104 MeV 16O on 142Nd, 144Sm, 148Sm and 152Sm

NUCLEAR REACTIONS 142Nd, 144,148,152Sm(16O, 14C), E=104 MeV; measured σ(E(14C), θ). 144Sm(16O, 12C), (16O, 13C), E=104 MeV; measured σ. 144Sm, 146,150,154Gd deduced levels.

1974BE16      Phys.Rev. C9, 1543 (1974)

F.D.Becchetti, D.G.Kovar, B.G.Harvey, D.L.Hendrie, H.Homeyer, J.Mahoney, W.von Oertzen, N.K.Glendenning

Two-Proton-Transfer Reactions 208Pb(12C, 10Be)210Po and 208Pb(16O, 14C)210Po

NUCLEAR REACTIONS 208Pb(12C, 10Be), (16O, 14C), E(12C)=78 MeV, E(16O)=104, 140 MeV; 209Bi(12C, 11B), (16O, 15N), E(12C)=78 MeV, E(16O)=104 MeV; measured σ(Eout, θ). 210Po levels deduced relative strengths.

doi: 10.1103/PhysRevC.9.1543
Citations: PlumX Metrics

1974CO36      Nucl.Phys. A234, 157 (1974)

J.Conrad, R.Repnow, E.Grosse, H.Homeyer, E.Jaeschke, J.P.Wurm

Quasi-Rotational Bands in Neutron Deficient Doubly Even Ba Isotopes

NUCLEAR REACTIONS 106,108,110Cd(16O, 2nγ), E=52.5-66 MeV; measured Eγ, Iγ, γγ, nγ, pγ, αγ-coincidences. 120,122,124Ba deduced levels, J, π. 120Ba deduced ground-state T1/2 upper limit. Enriched targets, Ge(Li) detectors.

doi: 10.1016/0375-9474(74)90384-4
Citations: PlumX Metrics

1974DE03      Phys.Rev.Lett. 32, 680 (1974)

R.M.DeVries, M.S.Zisman, J.G.Cramer, K.-L.Liu, F.D.Becchetti, B.G.Harvey, H.Homeyer, D.G.Kovar, J.Mahoney, W.von Oertzen

Observation of an Anomalous Angular Distribution in the Single-Nucleon - Transfer Reaction 12C(14N, 13N)13C at 100 MeV

NUCLEAR REACTIONS 12C(14N, 13N), E=100 MeV; measured σ(E(13N), θ). 13C deduced levels, L.

doi: 10.1103/PhysRevLett.32.680
Citations: PlumX Metrics

1973KO09      Phys.Rev.Lett. 30, 1075 (1973)

D.G.Kovar, B.G.Harvey, F.D.Becchetti, J.Mahoney, D.L.Hendrie, H.Homeyer, W.von Oertzen, M.A.Nagarajan

Evidence for Recoil Effects in Heavy-Ion Transfer Reactions

NUCLEAR REACTIONS 208Pb(12C, 11B), (16O, 15N), E(12C)=78 MeV, E(16O)=104, 140 MeV; measured σ(E(11B), E(15N), θ); deduced recoil effects. 209Bi levels deduced S.

doi: 10.1103/PhysRevLett.30.1075
Citations: PlumX Metrics

1972BR40      Phys.Rev.Lett. 29, 1261 (1972)

P.Braun-Munzinger, C.K.Gelbke, N.Grama, H.Homeyer, E.Ridinger, R.Stock

Excitation of Rotational Bands in 40Ca Observed in the Reaction 36Ar(16O, 12C)

NUCLEAR REACTIONS 36Ar(16O, 12C), E=45 MeV; measured σ(E(12C)). 40Ca deduced levels, rotational band structure.

doi: 10.1103/PhysRevLett.29.1261
Citations: PlumX Metrics

1972DU07      Phys.Lett. 38B, 306 (1972)

H.H.Duhm, N.Ueta, W.Heinecke, H.Hafner, H.Homeyer, P.D.Kunz

A Study of the 26Mg(6Li, 6He)26Al Charge Exchange Reactions

NUCLEAR REACTIONS 26Mg(6Li, 6Li), (6Li, 6He), E=36 MeV; measured σ(θ); deduced optical model parameters.

doi: 10.1016/0370-2693(72)90252-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1941.

1972FU16      Nucl.Phys. A196, 286 (1972)

H.Fuchs, H.Homeyer, H.Oeschler, R.Lipperheide, K.Mohring

Study of the Off-Energy-Shell n-15N Total Cross Section by Means of 15N(d, p) Stripping into the Continuum of 16N

NUCLEAR REACTIONS 15N(d, p), E=12.0 MeV; measured σ(Ep, θ). 16N deduced levels, J, π, S. Enriched target.

doi: 10.1016/0375-9474(72)90965-7
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1971FU14      Phys.Lett. 37B, 285 (1971)

H.Fuchs, H.Homeyer, T.Lorenz, H.Oeschler

Stripping into Unbound States: Interference between Resonant and Continuum States

NUCLEAR REACTIONS 15N(d, p), E=12 MeV; measured σ(Ep); deduced resonance interference. 16N deduced resonance.

doi: 10.1016/0370-2693(71)90020-7
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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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