NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = K.Hartmann Found 11 matches. 1990DU04 Phys.Rev.Lett. 65, 297 (1990) W.Dunnweber, W.Lippich, D.Otten, W.Assmann, K.Hartmann, W.Hering, D.Konnerth, W.Trombik Quantum-Statistical Interference of Coincident Neutrons from the Compound Nucleus NUCLEAR REACTIONS 26Mg(18O, xn), E=65, 88 MeV; measured nn-coin yields; deduced 44Ca evaporation chain average Γ.
doi: 10.1103/PhysRevLett.65.297
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
1983HA09 Z.Phys. A311, 131 (1983) Charge Transfer Prior to Fusion NUCLEAR REACTIONS 116Sn(35Cl, X), E=160-400 MeV; 208Pb(26Mg, X), E=150-250 MeV; measured σ(fusion) vs E.
doi: 10.1007/BF01411618
1982HA24 Nucl.Phys. A380, 170 (1982) K.M.Hartmann, W.Dunnweber, W.E.Frahn Partial Coherence in Heavy-Ion Reactions NUCLEAR REACTIONS 12C(16O, α), E=30 MeV; calculated cross correlation function; 12C(16O, α), E=29.6-32.7 MeV; 24Mg(α, α), E=14.9-19.1 MeV; calculated energy averaged σ(θ). Heavy ion reactions, partial coherence, interference effects.
doi: 10.1016/0375-9474(82)90588-7
1980DU04 Phys.Rev.Lett. 44, 729 (1980) Angular Correlation of Fast Light Particles and Heavy Ejectiles in Deep-Inelastic Heavy-Ion Reactions NUCLEAR REACTIONS Th(Ar, X), E=400 MeV; calculated HI(light fragment)(θ); deduced polarization P(HI) relation to correlation asymmetry.
doi: 10.1103/PhysRevLett.44.729
1980HA06 Z.Phys. A294, 65 (1980) On the Parametrized S-Matrix Approach to Deep Inelastic Collisions NUCLEAR REACTIONS 209Bi(136Xe, X), E=1130 MeV; calculated σ(fragment θ, Z). Parametrized S-matrix method to deep-inelastic collisions.
doi: 10.1007/BF01473122
1980HA48 Z.Phys. A297, 311 (1980) Direct Versus Thermal Particle Emission in High-Energy Heavy-Ion Collisions: Light fragment emission and the ratio of neutron to proton inclusive cross sections NUCLEAR REACTIONS U, Pb(20Ne, p), (20Ne, d), (20Ne, t), (20Ne, 3He), U(20Ne, α), E=400 MeV/nucleon; U(20Ne, n), E=300 MeV/nucleon; calculated σ(θp, Ep), σ(θd, Ed), σ(θt, Et), σ(θ(3He), E(3He)), σ(θα, Eα), σ(θn, En), neutron to proton inclusive yield ratio. Direct plus thermal component model.
doi: 10.1007/BF01422790
1979HA49 Phys.Lett. 87B, 21 (1979) Deep Inelastic Collisions Induced by Identical Heavy Ions NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E=284, 400 MeV; calculated σ(θ, Q).
doi: 10.1016/0370-2693(79)90007-8
1978HA28 Nucl.Phys. A305, 279 (1978) Lookng at DIC Through an l-Window NUCLEAR REACTIONS 232Th(40Ar, X), E=388 MeV; 209Bi(84Kr, X), E=600 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(78)90178-1
1977HA27 Z.Phys. A282, 293 (1977) Anomalous Large Angle Alpha Scattering NUCLEAR REACTIONS 40Ca(α, α), E=29 MeV; calculated σ(θ).
doi: 10.1007/BF01414897
1976HA42 Nucl.Phys. A269, 237 (1976) Diffractive, Refractive and Interference Effects in Heavy Ion Elastic Scattering NUCLEAR REACTIONS 40Ca(13C, 13C), E=40 MeV; 40Ca(16O, 16O), E=47 MeV; 40Ca(α, α), E=24 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(76)90409-7
Back to query form Note: The following list of authors and aliases matches the search parameter K.Hartmann: , K.M.HARTMANN, K.N.HARTMANN |