NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Fuchs Found 86 matches. 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
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
1998LE12 Phys.Rev. C57, 2375 (1998) X.Ledoux, H.G.Bohlen, J.Cugnon, H.Fuchs, J.Galin, B.Gatty, B.Gebauer, D.Guerreau, D.Hilscher, D.Jacquet, U.Jahnke, M.Josset, S.Leray, B.Lott, M.Morjean, B.M.Quednau, G.Roschert, H.Rossner, A.Peghaire, L.Pienkowski, R.H.Siemssen, C.Stephan Formation and Decay of Hot Nuclei in 475 MeV, 2 GeV Proton- and 2 GeV 3He-Induced Reactions on Ag, Bi, Au, and U NUCLEAR REACTIONS 107Ag, 197Au, 209Bi, 238U(p, X), E=0.475, 2 GeV; 107Ag, 197Au, 209Bi, 238U(3He, X), E=2 GeV; measured neutron multiplicity distributions, light-, intermediate-charged particle energy distributions, fission fragments; deduced compound nucleus temperature, other reaction mechanism features. Comparison with two-step cascade process model.
doi: 10.1103/PhysRevC.57.2375
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
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.
1994PI06 Acta Phys.Pol. B25, 737 (1994) L.Pienkowski, S.Leray, J.Galin, D.Guerreau, X.Ledoux, B.Lott, M.Morjean, A.Peghaire, H.-G.Bohlen, H.Fuchs, B.Gebauer, D.Hilscher, U.Jahnke, G.Roschert, H.Rossner, B.Gatty, D.Jacquet, C.Stephan, R.Siemssen, J.Cugnon Thermal Excitation Energy Distribution of 475 MeV and 2 GeV Proton and 3He Induced Reactions in Heavy Nuclei NUCLEAR REACTIONS U, 209Bi, 197Au, Ag(p, xn), E=0.475, 2 GeV; Ag, 197Au, 209Bi, U(3He, xn), E=2 GeV; measured neutron multiplicity distributions; deduced thermal excitation energy distribution. Intra-nuclear cascade model analysis.
1994PI08 Phys.Lett. 336B, 147 (1994) L.Pienkowski, H.G.Bohlen, J.Cugnon, H.Fuchs, J.Galin, B.Gatty, B.Gebauer, D.Guerreau, D.Hilscher, D.Jacquet, U.Jahnke, M.Josset, X.Ledoux, S.Leray, B.Lott, M.Morjean, A.Peghaire, G.Roschert, H.Rossner, R.H.Siemssen, C.Stephan Hot Nuclei in Reactions Induced by 475 MeV, 2 GeV 1H and 2 GeV 3He NUCLEAR REACTIONS Ag, 197Au, 209Bi, U(p, nX), E=0.475, 2 GeV; Ag, 197Au, 209Bi, U(3He, nX), E=2 GeV; measured inclusive neutron multiplicity distributions. Intranuclear cascade analysis.
doi: 10.1016/0370-2693(94)00910-4
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
1991BO15 Z.Phys. A338, 369 (1991) B.Borderie, M.F.Rivet, C.Cabot, H.Fuchs, D.Gardes, F.Hanappe, D.Jouan, M.Montoya Excitation Energy Partition in Deeply Inelastic Collisions between 40Ar and Ag at 27 MeV Per Nucleon NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured fragment particle evaporation; deduced excitation energy partition features.
doi: 10.1007/BF01288204
1991JO12 Z.Phys. A340, 63 (1991) D.Jouan, B.Borderie, M.F.Rivet, C.Cabot, H.Fuchs, H.Gauvin, C.Gregoire, F.Hanappe, D.Gardes, M.Montoya, B.Remaud, F.Sebille Dynamics and Thermalization in Violent Collisions between 40Ar and Ag at 27 MeV/nucleon NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured (fragment)(fragment)-coin; deduced reaction mechanism.
doi: 10.1007/BF01284482
1990EL04 Nucl.Phys. A517, 340 (1990) Y.El Masri, F.Hanappe, J.C.Steckmeyer, V.Martin, G.Bizard, B.Borderie, R.Brou, J.F.Bruandet, P.Duhamel, H.Fuchs, J.L.Laville, J.Peter, R.Regimbart, M.Rivet, B.Tamain, T.U.Chan Gamma-Ray Multiplicity Measurements for the Determination of the Initial Angular Momentum Ranges in Normal and Fast Fission Processes NUCLEAR REACTIONS 165Ho(40Ar, F), E=315 MeV; Re(20Ne, F), E=220 MeV; measured γ-multiplicity vs fission fragment mass, total kinetic energy; deduced fission mechanism, fragment mass distribution, critical angular momentum.
doi: 10.1016/0375-9474(90)90039-O
1990JA07 Nucl.Phys. A511, 195 (1990) D.Jacquet, G.F.Peaslee, J.M.Alexander, B.Borderie, E.Duek, J.Galin, D.Gardes, C.Gregoire, D.Guerreau, H.Fuchs, M.Lefort, M.F.Rivet, X.Tarrago Production and Deexcitation of Hot Nuclei in Collisions of 27 MeV/Nucleon 40Ar with 238U NUCLEAR REACTIONS 238U(40Ar, F), (40Ar, X), E=1080 MeV; measured (fragment)(fragment)-, (light charged particle)(fragment)-coin following fission. Landau-Vlasov calculations.
doi: 10.1016/0375-9474(90)90032-H
1988BO13 Phys.Lett. 205B, 26 (1988) B.Borderie, M.Montoya, M.F.Rivet, D.Jouan, C.Cabot, H.Fuchs, D.Gardes, H.Gauvin, D.Jacquet, F.Monnet, F.Hanappe Deeply Inelastic Collisions as a Source of Intermediate Mass Fragments at E/A = 27 MeV NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured fragment σ(θ1, θ2); deduced reaction mechanism.
doi: 10.1016/0370-2693(88)90393-0
1988RI06 Z.Phys. A330, 301 (1988) M.F.Rivet, R.Alami, B.Borderie, H.Fuchs, D.Gardes, H.Gauvin Fusion-Fission of Heavy Systems. Influence of the Entrance Channel Mass Asymmetry NUCLEAR REACTIONS 209Bi(40Ar, F), E=202, 238 MeV; 187Re(56Fe, F), E=294, 307, 326 MeV; measured fission σ, fragment mass distribution widths; deduced entrance channel role in fission.
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
1985MA02 Phys.Rev. C31, 443 (1985) H.Machner, D.Protic, G.Riepe, H.G.Bohlen, H.Fuchs Fast Light Particle Emission in 20 MeV/Nucleon 20Ne Induced Reactions NUCLEAR REACTIONS 197Au(20Ne, X), E=392 MeV; measured σ(E, θ) for X=p, d, t, 3,4,6He, 6,7,8,9Li; deduced model parameters. Moving source emission, preequilibrium, projectile breakup analyses.
doi: 10.1103/PhysRevC.31.443
1984FO02 Z.Phys. A315, 1 (1984) W.Foerster, K.D.Boklen, H.H.Fuchs, G.Nachtsheim, N.Sheta Detection of a Hexadecapole Interaction in the Atomic Ground State 3H6 of 167Er ATOMIC PHYSICS 167Er; measured Zeeman interactions, hfs; deduced Lande (g)-factor, ground state hyperfine separations. Atomic beam magnetic resonance method. NUCLEAR MOMENTS 167Er; measured hfs; deduced hyperfine, hexadecapole interaction constants, Lande (g)-factor. 167Er deduced multipole moments. Atomic beam magnetic resonance method.
doi: 10.1007/BF01436202
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
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
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
1981RO01 Z.Phys. A299, 73 (1981) J.C.Roynette, N.Frascaria, Y.Blumenfeld, J.C.Jacmart, E.Plagnol, J.P.Garron, A.Gamp, H.Fuchs Light Particle Coincidences with Gross Structure in Energy Spectra from the 40Ca + 40Ca Collision NUCLEAR REACTIONS 40Ca(40Ca, pX), 40Ca(40Ca, αX), E=400 MeV; measured σ(θp, θ(Ca)), σ(θp, θ(K)), σ(θα, θ(Ca)), σ(θα, θ(Ar)), σ(θp, fragment E, θ), σ(θα, fragment E, θ); deduced reaction mechanism, small evaporation decay.
doi: 10.1007/BF01415744
1980DA02 Z.Phys. A294, 289 (1980) M.Dakowski, R.Chechik, H.Fuchs, F.Hanappe, B.Lucas, C.Mazur, M.Morjean, J.Peter, M.Ribrag, C.Signarbieux, B.Tamain Evidence for Shape Deformations of Fragments in Deep Inelastic Collisions NUCLEAR REACTIONS 197Au(40Ar, X), E=240 MeV; measured n-emission ratio vs corresponding fragment A ratio, σ(En); deduced fragment shape deformation in deep-inelastic collisions. Monte Carlo calculations.
doi: 10.1007/BF01438169
1980FU04 Nucl.Phys. A343, 133 (1980) H.Fuchs, J.A.Nolen, G.J.Wagner, H.Lenske, G.Baur Experimental and Theoretical Study of Line Shapes in 13C(α, α') Inelastic Scattering to Resonant States NUCLEAR REACTIONS 13C(α, α'), E=22, 36 MeV; measured σ(Eα, θ). 13C resonance deduced line shape parameter. Enriched target.
doi: 10.1016/0375-9474(80)90645-4
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.
1979FU03 J.Phys.(London) G5, 797 (1979) H.Fuchs, T.S.Bhatia, P.Doll, H.Hafner, C.J.Wagner Experimental Study of Resonance Line-Shapes in 12C(τ, d) Stripping into the Continuum NUCLEAR REACTIONS 12C(3He, d), E=36.0 MeV; measured σ(Ed, θ); deduced reaction mechanism. 13N deduced levels.
doi: 10.1088/0305-4616/5/6/007
1979GA12 Z.Phys. A291, 347 (1979) A.Gamp, H.L.Harney, J.C.Roynette, E.Plagnol, H.Fuchs, H.Doubre, J.C.Jacmart, N.Poffe Out-of-Plane Correlations of α-Particles and Heavy Ions in the Reaction of 373 MeV 32S with Gold NUCLEAR REACTIONS 197Au(32S, X), E=373 MeV; measured σ(θ, φ) for P, S, Si+α, Al+α; deduced reaction mechanism.
doi: 10.1007/BF01408385
1979TA15 Nucl.Phys. A330, 253 (1979) B.Tamain, R.Chechik, H.Fuchs, F.Hanappe, M.Morjean, C.Ngo, J.Peter, M.Dakowski, B.Lucas, C.Mazur, M.Ribrag, C.Signarbieux Neutron Multiplicity in Deep Inelastic Collisions: 400 MeV Cu + Au System NUCLEAR REACTIONS 197Au(63Cu, X), E=400 MeV; (fragment) n-coin, fragment mass; neutron multiplicity, equilibration relaxation time.
doi: 10.1016/0375-9474(79)90549-9
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
1976BO17 Nucl.Phys. A263, 86 (1976) J.Bommer, M.Ekpo, H.Fuchs, K.Grabisch, H.Kluge Measurement of the Total Neutron Cross Section of 14N and 24Mg NUCLEAR REACTIONS 14N, 24Mg(n, X), E=1.0-5.2 MeV; measured σ(E). Enriched 24Mg target.
doi: 10.1016/0375-9474(76)90185-8
1976BO18 Nucl.Phys. A263, 93 (1976) J.Bommer, M.Ekpo, H.Fuchs, K.Grabisch, H.Kluge, H.Oeschler Stripping to Unbound States of 25Mg and 33S: Combined Analysis of (d, p) Spectra and the Total Neutron Cross Section of 24Mg and 32S NUCLEAR REACTIONS 24Mg, 32S(d, p), E=12 MeV; measured σ(Ep, θ), θ=10° or 12.5°. 25Mg, 33S deduced energy levels, J, L, π, Γ. Enriched 24Mg target.
doi: 10.1016/0375-9474(76)90186-X
1975AP01 Nucl.Phys. A246, 477 (1975) H.-J.Apell, W.Gemeinhardt, R.Stock, R.R.Betts, O.Hansen, A.Sperduto, H.Fuchs, R.Santo Anomalies in α-Scattering and (3He, α) Reactions on 40,41Ca and the Effect of Cluster Exchange NUCLEAR REACTIONS 40,41Ca(α, α), E=19, 24.1, 26.5 MeV; measured σ(θ). 40,41Ca(3He, α), E=16-27 MeV in 1 MeV steps; measured σ(Eα, θ). 39,40Ca levels deduced L, C2S. Radioactive 41Ca target.
doi: 10.1016/0375-9474(75)90660-0
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
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
1975BO32 Phys.Rev. C12, 1069 (1975) J.Bommer, M.Ekpo, H.Fuchs, K.Grabisch, H.Kluge Shape Parallelism of the Lowest Proton Resonance in 12C(p, p) and in 12C(d, n) NUCLEAR REACTIONS 12C(p, n), E=6.3 MeV; measured σ(En). 13N deduced peak shape.
doi: 10.1103/PhysRevC.12.1069
1975BO33 Z.Phys. A274, 195 (1975) K.D.Boklen, T.Bossert, W.Foerster, H.H.Fuchs, G.Nachtsheim Hyperfine Structure Measurements in the 4I9/2 Ground State of 141Pr NUCLEAR MOMENTS 141Pr; measured hfs.
1975BO34 Nucl.Phys. A251, 246 (1975) J.Bommer, M.Ekpo, H.Fuchs, K.Grabisch, H.Kluge Spectroscopic Study of 15N States with the Reaction 14C(d, n) NUCLEAR REACTIONS 14C(d, n), E=6.5 MeV; measured σ(En, θ). 15N levels deduced L, J, π, S. Enriched target.
doi: 10.1016/0375-9474(75)90068-8
1975BO35 Nucl.Phys. A251, 257 (1975) J.Bommer, M.Ekpo, H.Fuchs, K.Grabisch, H.Kluge Stripping to Unbound States of 13-15N: Combined Analysis of (d, n) and (p, p0) on 12-14C NUCLEAR REACTIONS 12,13,14C(d, n), E=6.3 or 6.5 MeV; measured σ(En, θ). 13,14,15N levels deduced, L, J, π, S. Enriched 13,14C targets.
doi: 10.1016/0375-9474(75)90069-X
1974BO34 Phys.Lett. 52B, 421 (1974) J.Bommer, M.Ekpo, H.Fuchs, K.Grabisch, H.Oeschler Determination of the l-Value of Nucleon Resonances from their Formation in Deuteron Stripping and Comparison with the Total Nucleon Cross Section NUCLEAR REACTIONS 32S, 24Mg(d, p), E=12 MeV; measured σ(Ep). 24Mg(n, X), E=1-5.2 MeV; measured total σ(E, En). 12,13,14C(d, n); measured σ(E, En). 25Mg, 13,14,15N resonances deduced L.
doi: 10.1016/0370-2693(74)90115-4
1974FU07 Phys.Lett. 49B, 447 (1974) H.Fuchs, K.Grabisch, D.Hilscher, U.Jahnke, H.Kluge, T.G.Masterson, H.Morgenstern Evidence for Quadrupole Pairing in 56Ni NUCLEAR REACTIONS 54Fe(3He, n), E(3He)=13.0 MeV; measured σ(En, θ). 56Ni deduced levels, J, π, L.
doi: 10.1016/0370-2693(74)90632-7
1974FU11 Nucl.Phys. A234, 61 (1974) H.Fuchs, K.Grabisch, D.Hilscher, U.Jahnke, H.Kluge, T.Masterson, H.Morgenstern Investigation of the Shell Model Structure of States in 11C and 12N with the (3He, n) Reaction on 9Be and 10B NUCLEAR REACTIONS 9Be, 10B(3He, n), E=10.5-13 MeV; measured σ(E, En, θ). 11C, 12N deduced levels, L, J, π, analog states.
doi: 10.1016/0375-9474(74)90379-0
1973BO02 Nucl.Phys. A199, 115 (1973) J.Bommer, H.Fuchs, K.Grabisch, H.Kluge, W.Ribbe, G.Roschert Study of 59Cu by Means of 58Ni(d, n) NUCLEAR REACTIONS 58Ni(d, n), Ed=7.0 MeV; measured σ(En, θ). 59Cu deduced levels, L, S. Enriched target.
doi: 10.1016/0375-9474(73)90337-0
1973BO03 Nucl.Phys. A199, 121 (1973) J.Bommer, B.Efken, H.Fuchs, K.Grabisch, H.Kluge, W.Ribbe, G.Roschert, F.Sichelschmidt Optical Potential of 58Ni for Low-Energy Deuterons from the Sub-Coulomb (d, n) Reaction NUCLEAR REACTIONS 58Ni(d, n), Ed=4.0-7.0 MeV; measured σ(E;En, θ); deduced deuteron potential parameters. Enriched target.
doi: 10.1016/0375-9474(73)90338-2
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
1973FU02 Nucl.Phys. A202, 396 (1973) Energy Dependence of Transition Strengths Extracted from 12C(3He, α) and 16O(3He, α) NUCLEAR REACTIONS 12C, 16O(3He, α), E=24, 28 MeV; measured σ(Eα, θ); 11C, 15O deduced L, S. Natural targets.
doi: 10.1016/0375-9474(73)90232-7
1973OE01 Nucl.Phys. A202, 513 (1973) H.Oeschler, H.Fuchs, H.Schroter Study of Enhanced Backward α-Scattering on Nuclei with A=12-18 NUCLEAR REACTIONS 12,14C, 15N, 16,18O(α, α), E=22-29 MeV; measured σ(E, θ); deduced Regge-pole parameters. Enriched targets.
doi: 10.1016/0375-9474(73)90639-8
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
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
1972OE01 Phys.Rev.Lett. 28, 694 (1972) H.Oeschler, H.Schroter, H.Fuchs, L.Baum, G.Gaul, H.Ludecke, R.Santo, R.Stock Shell-Structure Effect on Elastic α Scattering NUCLEAR REACTIONS 12,14C, 14,15N, 16,18O, 32,34S, 36,38,40Ar, 39,40,41K, 40,42,44,48Ca(α, α), (α, α'), E=24, 29 MeV; measured σ(θ); deduced back-angle enhancements, shell structure effects.
doi: 10.1103/PhysRevLett.28.694
1971BO04 Nucl.Phys. A160, 577 (1971) J.Bommer, K.Grabisch, H.Kluge, G.Roschert, H.Fuchs, U.Lynen, K.K.Seth Study of 43Sc States with Proton Transfer Reactions on 42Ca NUCLEAR REACTIONS 42Ca(d, n), E=5.0-6.05 MeV;42Ca(3He, d), E=18 MeV; measured σ(E, θ). 43Sc deduced levels, isobaric analogs, L, J, π, S. Enriched 42Ca targets.
doi: 10.1016/0375-9474(71)90099-6
1971BO33 Nucl.Phys. A173, 383 (1971) J.Bommer, H.Fuchs, K.Grabisch, H.Kluge, G.Roschert Spectroscopy of 93,95Tc by Means of 92,94Mo(d, n) NUCLEAR REACTIONS 92,94Mo(d, n), Ed=6.25, 7.0 MeV; measured σ(E, θ). 93,95Tc deduced level energies, L, J, π, S. Enriched 92,94Mo targets.
doi: 10.1016/0375-9474(71)90351-4
1971BO35 Nucl.Phys. A172, 618 (1971) J.Bommer, H.Fuchs, K.Grabisch, U.Janetzki, G.Roschert Study of 15O States by the 14N(d, n) Reaction NUCLEAR REACTIONS 14N(d, n), E=5.6, 6.0 MeV; measured σ(En, θ). 15O deduced levels, L, S. Natural targets.
doi: 10.1016/0375-9474(71)90048-0
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
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
1970FU01 Phys.Lett. 31B, 14 (1970) H.Fuchs, M.Hagen, U.Janetzki, K.-H.Maier Observation of Target Ground State Correlations in the (d, n) Reactions On Even Argon Isotopes NUCLEAR REACTIONS 36,38,40Ar(d, n), E=5.6 MeV; measured σ(En, θ). 37,39,41K levels deduced S.
doi: 10.1016/0370-2693(70)90007-9
1970HA37 Nucl.Phys. A152, 404 (1970) M.Hagen, U.Janetzki, K.-H.Maier, H.Fuchs The (d, n) Reactions on Even Argon Isotopes NUCLEAR REACTIONS 36,38,40Ar(d, n), E=5.6 MeV; measured σ(En, θ). 37,39,41K deduced levels, L, π, J, S, t. Enriched 36,38Ar targets.
doi: 10.1016/0375-9474(70)90841-9
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
1969FU01 Nucl.Phys. A129, 545 (1969) H.Fuchs, K.Grabisch, G.Roschert Investigation of States in 40Ca by the 39K(d, n) Reaction NUCLEAR REACTIONS 39K(d, n), E=6 MeV; measured σ(En, θ). 40Ca deduced levels, L, π, S, T. Natural target.
doi: 10.1016/0375-9474(69)90700-3
1969FU06 Nucl.Phys. A133, 385 (1969) H.Fuchs, K.Grabisch, G.Roschert The 60Ni(d, n) Reaction above and below the Coulomb Barrier and the Deuteron Optical-Model Potential NUCLEAR REACTIONS 60Ni(d, n), E = 3.8-6 MeV; measured σ(E; En, θ);deduced optical-model parameters. 61Cu deduced levels, L, S. Enriched target.
doi: 10.1016/0375-9474(69)90640-X
1968FU03 Nucl.Phys. A110, 65(1968) H.Fuchs, K.Grabisch, P.Kraaz, G.Roschert Study of States in 25Al and 26Al by the 24Mg(d, n) and 25Mg(d, n) Reactions NUCLEAR REACTIONS 24,25Mg(d, n), Ed=5.5 or 6 MeV; measured σ(En, θ). 25,26Al deduced levels, L, π, J, T, S. Enriched targets.
doi: 10.1016/0375-9474(68)90683-0
1968FU10 Nucl.Phys. A122, 59(1968) H.Fuchs, K.Grabisch, P.Kraaz, G.Roschert Study of 24Mg by the 23Na(d, n) Reaction at E = 6 MeV NUCLEAR REACTIONS 23Na(d, n), E=6 MeV; measured σ(En, θ). 24Mg deduced levels, L, π, S, T. Natural target.
doi: 10.1016/0375-9474(68)90702-1
1967FU04 Phys.Letters 24B, 234 (1967) Indications for Isospin Dependence of Angular Distributions in Nucleon Transfer Reactions NUCLEAR STRUCTURE 11B, 9Be, 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90472-8
1967FU06 Phys.Letters 25B, 204 (1967) H.Fuchs, K.Grabisch, P.Kraaz, G.Roschert Contribution to Subcoulomb Stripping: The Reaction 116Sn(d, n)117Sb at 6 MeV NUCLEAR STRUCTURE 117Sb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90037-8
1967FU07 Nucl.Phys. A105, 590(1967) H.Fuchs, K.Grabisch, P.Kraaz, G.Roschert States in 12C and 16O Investigated by the 11B(d, n) and 15N(d, n) Reactions NUCLEAR REACTIONS 11B(d, n), 15N(d, n), E=6 MeV; measured σ(En, θ). 12C, 16O deduced levels, L, S. Enriched targets.
doi: 10.1016/0375-9474(67)90537-4
1966FU10 Phys.Letters 23, 363 (1966) H.Fuchs, K.Grabisch, P.Kraaz, G.Roschert Shell Model Configurations of States in 14N Studies by the 13C(d, n)14N Reaction NUCLEAR STRUCTURE 14N, 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90468-9
1966SI02 Phys.Rev.Letters 16, 1050 (1966) R.H.Siemssen, G.C.Morrison, B.Zeidman, H.Fuchs Discrepancies in Proton-Transfer Reactions to States with Different Isobaric Spin NUCLEAR STRUCTURE 13C, 14N, 10B, 9Be, 26Al; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.16.1050
1965FU05 Nucl.Phys. 66, 638 (1965) The Probability for Transitions Between the First 2+ and the First 0+ Excited States of O16 NUCLEAR REACTIONS 19F(p, αγ), E = 0.874 MeV; measured γ(E+E-)-coin. 16O deduced B(E2), deformation parameter.
doi: 10.1016/0029-5582(65)90791-1
1963FU05 Z.Physik 171, 403 (1963) Die Spektren der Neutronen aus Den Reaktionen C12(y, n)C11 und O16(y, n)O15 NUCLEAR STRUCTURE 12C, 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01380658
1963FU06 Z.Physik 171, 416 (1963) Die Spektren der Photoneutronen aus O18 und N14 NUCLEAR STRUCTURE 14N, 18O; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01380659
1962FU11 Z.Naturforsch. 17a, 439 (1962) H.Fuchs, D.Haag, K.H.Lindenberger, U.Meyer-Berkhout NUCLEAR STRUCTURE 12C, 16O; measured not abstracted; deduced nuclear properties.
1961BR28 Z.Physik 165, 485 (1961) P.Brix, H.Fuchs, K.H.Lindenberger, C.Salander Relativmessung integrierter Wirkungsquerschnitte fur den Kernphotoeffekt: Die Reaktion O16(γ, n)O15 NUCLEAR REACTIONS 16O(γ, n), E<34 MeV; measured reaction products; deduced yields, integrated σ ratios. <DOI >10.1007/BF01377812
1960FU07 Contrib.Karlsruhe Photonuclear Conf., Karlsruhe, Germany, Paper A11 (1960) A Measurement of the Integrated Cross Section of the O16(γ, n)O15 Reaction NUCLEAR STRUCTURE 12C, 16O; measured not abstracted; deduced nuclear properties.
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