NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = J.Buschmann Found 18 matches. 1989GI01 Nucl.Instrum.Methods Phys.Res. A276, 169 (1989) H.J.Gils, H.Jelitto, H.Schlosser, S.Zagromski, J.Buschmann, W.Eyrich, A.Hofmann, J.Kiener, A.Lehmann, H.Rebel The QQDS Magnetic Spectrograph ' Little John ' at the Karlsruhe Cyclotron II. Experimental procedures and performance NUCLEAR REACTIONS 12C(6Li, 6Li), E=158 MeV; measured 6Li spectra. 208Pb, 12C(6Li, αX), E=156 MeV; measured σ(θα, Eα). 12C(6Li, 6Li'), E=156 MeV; measured σ(θ), σ(θ(6Li), E(6Li)). 12C(6Li, 6He), E=156 MeV; measured σ(θ(6He), E(6He)).
doi: 10.1016/0168-9002(89)90629-3
1989JE01 Z.Phys. A332, 317 (1989) H.Jelitto, J.Buschmann, V.Corcalciuc, H.J.Gils, N.Heide, J.Kiener, H.Rebel, C.Samanta, S.Zagromski Inclusive Measurements of the Break-Up of 156 MeV 6Li-Ions at Extreme Forward Angles NUCLEAR REACTIONS 12C, 208Pb(6Li, αX), (6Li, dX), E=156 MeV; measured σ(θα), σ(θd), inclusive reaction σ(θα, Eα), σ(θd, Ed); deduced reaction, projectile breakup mechanisms.
1987KO15 Z.Phys. A326, 421 (1987) T.Kozik, J.Buschmann, K.Grotowski, H.J.Gils, N.Heide, J.Kiener, H.Klewe-Nebenius, H.Rebel, S.Zagromski, A.J.Cole, S.Micek Intermediate Mass Fragments in the Reaction 6Li + 46Ti at E/A = 26 MeV NUCLEAR REACTIONS 46Ti(6Li, X), E=156 MeV; measured σ(fragment θ, E) for fragment Z=4-11; deduced reaction mechanism. Enriched target, ΔE-E telescopes. Binary decay model.
1986PL01 Nucl.Phys. A448, 110 (1986) R.Planeta, H.Klewe-Nebenius, J.Buschmann, H.J.Gils, H.Rebel, S.Zagromski, T.Kozik, L.Freindl, K.Grotowski The Nonelastic Projectile Break-Up Cross Section from Particle-Gamma Coincidence Measurements for the 6Li + 40Ca Reaction at 156 MeV NUCLEAR REACTIONS 40Ca(6Li, α), (6Li, 3He), (6Li, t), (6Li, d), (6Li, p), E=156 MeV; measured (fragment)γ-coin following breakup, inclusive, exclusive reactions; deduced projectile breakup σ.
doi: 10.1016/0375-9474(86)90183-1
1984BR04 Nucl.Phys. A417, 174 (1984) J.Brzychczyk, L.Freindl, K.Grotowski, Z.Majka, S.Micek, R.Planeta, M.Albinska, J.Buschmann, H.Klewe-Nebenius, H.J.Gils, H.Rebel, S.Zagromski Fusion and Nonfusion Phenomena in the 6Li + 40Ca Reaction at 156 MeV NUCLEAR REACTIONS 40Ca(6Li, X), (6Li, γ), E=156 MeV; measured σ(fragment θ, E), σ(fragment Z); deduced projectile breakup. Calculated σ(fusion).
doi: 10.1016/0375-9474(84)90329-4
1983PE10 Z.Phys. A313, 111 (1983) R.Pesl, H.J.Gils, H.Rebel, E.Friedman, J.Buschmann, H.Klewe-Nebenius, S.Zagromski Optical Potentials and Isoscalar Transition Rates from 104 MeV Alpha-Particle Scattering by the N = 28 Isotones 48Ca, 50Ti and 52Cr NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr(α, α), (α, α'), E=104 MeV; measured σ(θ); deduced optical model, deformation parameters. 50Ti, 52Cr deduced rms charge radii, isoscalar transition rates. 48Ca deduced rms charge radii.
doi: 10.1007/BF02115849
1982CO09 Z.Phys. A305, 351 (1982) V.Corcalciuc, H.J.Gils, H.Rebel, J.Buschmann, R.Pesl, R.Dumitrescu, S.Zagromski, K.Feisst 104 MeV Alpha Particle Scattering from 90,92Zr NUCLEAR REACTIONS 90,92Zr(α, α), (α, α'), E=104 MeV; measured σ(θ). 90,92Zr deduced isoscalar quadrupole, hexadecapole transition rates. Anharmonic vibrator model, coupled-channels method.
doi: 10.1007/BF01419085
1982NE02 Nucl.Phys. A382, 296 (1982) B.Neumann, H.Rebel, H.J.Gils, R.Planeta, J.Buschmann, H.Klewe-Nebenius, S.Zagromski, R.Shyam, H.Machner Inclusive Break-Up Reactions of 6Li at an Incident Energy of 26 MeV/Nucleon NUCLEAR REACTIONS 40Ca(6Li, p), (6Li, d), (6Li, t), (6Li, 3He), (6Li, α), E=156 MeV; measured σ(θ) versus particle energy. DWBA, breakup, preequilibrium exciton coalescence models.
doi: 10.1016/0375-9474(82)90138-5
1980GI02 Phys.Rev. C21, 1239 (1980) H.J.Gils, E.Friedman, H.Rebel, J.Buschmann, S.Zagromski, H.Klewe-Nebenius, B.Neumann, R.Peel, G.Bechtold Nuclear Sizes of 40,42,44,48Ca from Elastic Scattering of 104 MeV Alpha Particles. I. Experimental Results and Optical Potentials NUCLEAR REACTIONS 40,42,44,48Ca(α, α), E=104 MeV; measured σ(θ); deduced real potential isotopic dependence. Optical model analysis, Fourier-Bessel method.
doi: 10.1103/PhysRevC.21.1239
1980NE05 Z.Phys. A296, 113 (1980) B.Neumann, H.Rebel, J.Buschmann, H.J.Gils, H.Klewe-Nebenius, S.Zagromski Projectile Break-Up in Continuous Particle Spectra from Nuclear Reactions Induced by 156 MeV 6Li NUCLEAR REACTIONS 12C, 60Ni, 90Zr, 120Sn, 208Pb(6Li, p), (6Li, d), (6Li, 3He), (6Li, α), E=156 MeV; measured σ(θ, Ep), σ(θ, Ed), σ(θ, E(3He)), σ(θ, Eα), projectile breakup; deduced reaction mechanism, cluster momentum distribution. Plane wave model.
doi: 10.1007/BF01412652
1979NE06 Nucl. Phys. A329, 259 (1979) B.Neumann, J.Buschmann, H.Klewe-Nebenius, H.Rebel, H.J.Gils Transfer of 6Li Break-up Fragments at 6Li Projectile Energies Far Above the Coulomb Barrier NUCLEAR REACTIONS 208Pb, 209Bi(6Li, xnyp), (6Li, xnd), E=60-156 MeV; measured σ(E), recoil ranges.
doi: 10.1016/0375-9474(79)90293-8
1978FA03 J.Phys.(London) G4, 247 (1978) H.Faust, A.Hanser, H.Klewe-Nebenius, H.Rebel, J.Buschmann, H.J.Gils Experimental Studies of Hexadecapole Motion in Spherical Nuclei RADIOACTIVITY 60Co, 140La; measured γ-spectrum. 60Ni, 140Ce deduced E4 transitions. NUCLEAR REACTIONS 60Ni, 140Ce(α, α'γ), E=104 MeV; measured γ-spectrum, σ(Eα'). 60Ni, 140Ce levels deduced L, B(E4), β.
doi: 10.1088/0305-4616/4/2/014
1977GI08 Phys.Lett. 68B, 427 (1977) H.J.Gils, H.Rebel, J.Buschmann, H.Klewe-Nebenius Giant Resonance Excitation by 156 MeV 6Li Scattering NUCLEAR REACTIONS 208Pb(6Li, 6Li'), E=156 MeV; measured σ(E(6Li'), θ). 208Pb deduced giant resonance.
doi: 10.1016/0370-2693(77)90460-9
1977KR01 Z.Phys. A280, 61 (1977) J.Kropp, H.Klewe-Nebenius, H.Faust, J.Buschmann, H.Rebel, H.J.Gils, K.Wisshak Excitation Functions of 191+193Ir, 197Au(6Li, xn+yp) Compound Nuclear Reactions at E = 48-156 MeV NUCLEAR REACTIONS 191,193Ir, 197Au(6Li, xnyp), X=3-13, y=0-2, E=48-156 MeV; measured σ(E).
doi: 10.1007/BF01438110
1976GI10 Z.Phys. A279, 55 (1976) H.J.Gils, H.Rebel, J.Buschmann, H.Klewe-Nebenius, G.P.Nowicki, W.Nowatzke Nuclear Matter Sizes and Isoscalar Octupole Transition Rates of 204,206,208Pb from 104 MeV α-Particle Scattering NUCLEAR REACTIONS 204,206,208Pb(α, α), (α, α'), E=104 MeV; measured σ(θ). 204,206,208Pb deduced rms radii, isoscalar octupole transition probabilities. Folding model analysis.
doi: 10.1007/BF01409092
1976WI09 Z.Phys. A277, 129 (1976) K.Wisshak, A.Hanser, H.Klewe-Nebenius, J.Buschmann, H.Rebel, H.Faust Experimental Studies of the Level Scheme of 143Eu and a Generalized Decoupling Model Description RADIOACTIVITY 143mGd; measured Eγ, Iγ, γγ-coin, T1/2; deduced log ft, ICC. 143Eu deduced levels, J, π, λ. NUCLEAR REACTIONS 144Sm(α, 4npγ), E=75-120 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), γ(t). 143Eu deduced levels, J, π, T1/2, γ-branching.
doi: 10.1007/BF01433704
1975NO08 Nucl.Phys. A249, 76 (1975) G.P.Nowicki, J.Buschmann, A.Hanser, H.Rebel, H.Faust, D.Habs, H.Klewe-Nebenius, K.Wisshak The Level Scheme of 137Nd from (α, xn) Reactions and from β-Decay of The 11/2- Isomer of 137Pm RADIOACTIVITY 137Pm [from 141Pr(α, 8n)]; measured Eγ, Iγ, γγ-coin, E(ce), I(ce); deduced ICC. 137Nd deduced levels, J, π. Natural target, mass-separated sources, Ge(Li) detectors, Si(Li) detector with magnetic filter. NUCLEAR REACTIONS 140Ce(α, 7n), E=80-104 MeV; measured σ(E, Eγ, θ), γγcoin, E(ce), I(ce)(θ). 137Nd deduced levels, J, π. Natural target, Ge(Li) detectors, Si(Li) detector with magnetic filter.
doi: 10.1016/0375-9474(75)90092-5
1970GI02 Nucl.Phys. A145, 337 (1970) J.Gindler, H.Munzel, J.Buschmann, G.Christaller, F.Michel, G.Rohde Fragment Angular Distributions in the Fission of Heavy Nuclei by 103 MeV Helium Ions and 51.5 MeV Deuterons NUCLEAR REACTIONS, Fission 197Au, 209Bi, 233,234,235,238U(α, F), E=103 MeV; 209Bi, 233,234,235,238U(d, F), E=51.5 MeV; measured fission fragment σ(θ), σ(α), F, σ(d), F. Enriched targets.
doi: 10.1016/0375-9474(70)90427-6
Back to query form |