NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = H.Homeyer Found 52 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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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