NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.J.Gils Found 57 matches. 1999AN44 J.Phys.(London) G25, 2161 (1999) T.Antoni, W.D.Apel, K.Bekk, K.Bernlohr, E.Bollmann, K.Daumiller, P.Doll, J.Engler, F.Fessler, H.J.Gils, R.Glasstetter, R.Haeusler, W.Hafemann, A.Haungs, D.Heck, J.R.Horandel, T.Holst, K.-H.Kampert, H.O.Klages, J.Knapp, H.J.Mathes, H.J.Mayer, J.Milke, D.Muhlenberg, J.Oehlschlager, H.Rebel, M.Risse, M.Roth, G.Schatz, H.Schieler, F.K.Schmidt, T.Thouw, H.Ulrich, J.Unger, J.H.Weber, J.Wentz, T.Wiegert, D.Wochele, J.Kempa, T.Wibig, J.Zabierowski, F.Badea, H.Bozdog, I.M.Brancis, M.Petcu, B.Vulpescu, A.Chilingarian, A.Vardanyan Test of High-Energy Interaction Models using the Hadronic Core of EAS
1998MO01 Phys.Rev. C57, 602 (1998) M.Moosburger, E.Aschenauer, H.Dennert, W.Eyrich, A.Lehmann, N.Scholz, H.Wirth, H.J.Gils, H.Rebel, S.Zagromski Excitation and Decay of the Gamow-Teller Giant Resonance in 90Nb NUCLEAR REACTIONS 90Zr(6Li, 6He), E=156 MeV; measured σ(θ), p(6He)-coin following residual nucleus decay. 90Nb deduced Gamow-Teller giant resonance E, Γ, decay branching ratios, statistical damping.
doi: 10.1103/PhysRevC.57.602
1995DE53 Phys.Rev. C52, 3195 (1995) H.Dennert, E.Aschenauer, W.Eyrich, A.Lehmann, M.Moosburger, N.Scholz, H.Wirth, H.J.Gils, H.Rebel, S.Zagromski Excitation of Giant Monopole Resonance in 24Mg using 6Li Scattering NUCLEAR REACTIONS 24Mg(6Li, 6Li'), E=156 MeV; measured σ(θ) at extreme forward angles. 24Mg deduced electric giant monopole resonance, strength distribution, centroid energy, width, sum rule values. DWBA calculations.
doi: 10.1103/PhysRevC.52.3195
1993SC02 Z.Phys. A344, 269 (1993) N.Scholz, E.Aschenauer, H.Dennert, W.Eyrich, A.Lehmann, M.Moosburger, H.Wirth, H.J.Gils, H.Rebel, S.Zagromski Proton Decay of Spin Isospin Modes Excited by the 12C(6Li, 6He)12N Reaction NUCLEAR REACTIONS 12C(6Li, 6He), (6Li, p6He), E=156 MeV; measured particle spectra, p(6He)-coin, σ(θp, θ(6He)). 12N levels deduced proton decay spin, isospin modes features.
doi: 10.1007/BF01303020
1992PA20 Rev.Roum.Phys. 37, 121 (1992) M.Parlog, D.Popescu, J.Wentz, S.Zagromski, I.M.Brancus, V.Corcalciuc, M.Duma, H.J.Gils, H.Rebel Intermediate Mass Fragment Emission in 104 MeV α + 46-Ti Reactions NUCLEAR REACTIONS 46Ti(α, X), E=104 MeV; measured σ(fragment θ, E), σ vs charge number; deduced intermediate fragment emission mechanism. Extended sum rule model analysis.
1991AS05 Phys.Rev. C44, 2771 (1991) E.Aschenauer, H.Dennert, W.Eyrich, A.Lehmann, M.Moosburger, H.Wirth, H.J.Gils, H.Rebel, S.Zagromski (6Li, 6He) Measurements as an Alternative Calibration for Solar Neutrino Detectors NUCLEAR REACTIONS 37Cl, 71Ga(6Li, 6He), E=156 MeV; measured σ(θ) vs E. 37Ar, 71Ge level deduced Gamow-Teller transition strength distribution. Solar neutrino detectors targets, magnetic spectrograph.
doi: 10.1103/PhysRevC.44.2771
1991KI05 Z.Phys. A339, 489 (1991) J.Kiener, G.Gsottschneider, H.J.Gils, H.Rebel, V.Corcalciuc, S.K.Basu, G.Baur, J.Raynal Investigation of Sequential Break-Up Mode 6Li → 6Li(*) (3+1) → α + d of 156 MeV 6Li Projectiles on 208Pb in the Very Forward Angular Hemisphere NUCLEAR REACTIONS 208Pb(6Li, 6Li), (6Li, 6Li'), E=156 MeV; measured σ(θ), dα-coin following projectile breakup; deduced breakup mechanism.
doi: 10.1007/BF01288432
1991KI07 Phys.Rev. C44, 2195 (1991) J.Kiener, H.J.Gils, H.Rebel, S.Zagromski, G.Gsottschneider, N.Heide, H.Jelitto, J.Wentz, G.Baur Measurements of the Coulomb Dissociation Cross Section of 156 MeV 6Li Projectiles at Extremely Low Relative Fragment Energies of Astrophysical Interest NUCLEAR REACTIONS 208Pb(6Li, dα), E=156 MeV; measured σ(θα, θd, E(dα)); deduced radiative capture σ, astrophysical S-factor. Coincidence measurements with magnetic spectrometer.
doi: 10.1103/PhysRevC.44.2195
1990MO13 Phys.Rev. C41, 2925 (1990) M.Moosburger, E.Aschenauer, H.Dennert, W.Eyrich, A.Lehmann, R.Rudeloff, H.Schlosser, H.Wirth, H.J.Gils, H.Rebel, S.Zagromski (6Li, 6He) Reaction and Gamow-Teller β Decay NUCLEAR REACTIONS 12C, 18O, 26Mg, 42Ca(6Li, 6He), E=156 MeV; measured σ(E, θ), σ(θ=0°); deduced relation between Gamow-Teller transition strength (β-decay), zero degree cross section. DWBA calculations. Magnetic spectrograph.
doi: 10.1103/PhysRevC.41.2925
1990SR02 Z.Phys. A335, 417 (1990) D.K.Srivastava, D.N.Basu, H.Rebel, H.J.Gils Orbital Dispersion and Wavefunction Mapping in Inclusive Break-Up Experiments NUCLEAR REACTIONS 12C, 208Pb(6Li, αX), E=26 MeV/nucleon; analyzed σ(θα, Eα); deduced projectile internal momentum distribution.
1990WI08 Phys.Rev. C41, 2698 (1990) H.Wirth, E.Aschenauer, W.Eyrich, A.Lehmann, M.Moosburger, H.Schlosser, H.J.Gils, H.Rebel, S.Zagromski Investigation of Spin-Isospin Strength in 48Ca → 48Sc and 90Zr → 90Nb Using the (6Li, 6He) Reaction NUCLEAR REACTIONS 90Zr, 48Ca(6Li, 6He), E=156 MeV; measured σ(E, θ). 48Sc, 90Nb deduced Gamow-Teller strength, sum rule values. DWBA calculations. Magnetic spectrograph.
doi: 10.1103/PhysRevC.41.2698
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
1989HE28 Nucl.Phys. A504, 374 (1989) N.Heide, H.Rebel, V.Corcalciuc, H.J.Gils, H.Jelitto, J.Kiener, J.Wentz, S.Zagromski, D.K.Srivastava Elastic Break-Up of 156 MeV 6Li Projectiles with Large Asymptotic Relative Momenta of the Fragments: Experimental observations and the diffractive disintegration approach NUCLEAR REACTIONS 12C, 208Pb(6Li, dα), E=156 MeV; measured σ(θd, θα, Eα). Diffractive dissociation model analysis.
doi: 10.1016/0375-9474(89)90352-7
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.
1989KI07 Z.Phys. A332, 359 (1989) J.Kiener, H.J.Gils, H.Rebel, G.Baur Observation of Nonresonant Coulomb Break-Up of 156 MeV 6Li Projectiles NUCLEAR REACTIONS 208Pb(6Li, dα), E=156 MeV; measured σ(θ(6Li), θ(αd), E(αd)); deduced projectile breakup mechanism.
1987EY01 Phys.Rev. C36, 416 (1987) W.Eyrich, A.Hofmann, A.Lehmann, B.Muhldorfer, H.Schlosser, H.Wirth, H.J.Gils, H.Rebel, S.Zagromski E0 Strength in 12C from 6Li Scattering NUCLEAR REACTIONS 12C(6Li, 6Li'), E=156 MeV; measured σ(E(6Li), θ), θ=0°-2.5°. 12C deduced E0 transition strength distribution, EWSR fraction. DWBA analysis.
doi: 10.1103/PhysRevC.36.416
1987GI06 Nucl.Phys. A473, 111 (1987) Density Dependent Effective Interactions in Double-Folding Model Analyses of Elastic α-Particle Scattering NUCLEAR REACTIONS 40Ca, 50Ti, 52Cr(α, α), E=104 MeV; 40Ca, 50Ti(α, α), E=140 MeV; calculated model parameter characteristics. 40Ca(α, α), E=104 MeV; calculated σ(θ). Phenomenological density dependent effective interaction, double folding model.
doi: 10.1016/0375-9474(87)90157-6
1987JE03 Rev.Roum.Phys. 32, 629 (1987) H.Jelitto, H.J.Gils, H.Rebel, S.Zagromski Measurements of Light Particle Emission at very Forward Angles in 6Li Induced Nuclear Reactions at 26 MeV per Nucleon NUCLEAR REACTIONS, MECPD 12C, 208Pb(6Li, X), 208Pb(6Li, dα), E=156 MeV; measured light fragment σ(E(X), θ(X)), σ(θ(X)), αd-coin. Magnetic spectrograph.
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.
1987MI34 Z.Phys. A328, 467 (1987) S.Micek, H.Rebel, H.J.Gils, H.Klewe-Nebenius, S.Zagromski, D.K.Srivastava Single Nucleon Transfer Reactions in 6Li + 6Li Collisions at 156 MeV NUCLEAR REACTIONS, MECPD 6Li(6Li, 7Li), (6Li, 7Be), E=156 MeV; measured σ(E(7Li)), σ(E(7Be)), σ(θ); deduced model parameters. Finite range DWBA calculations.
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
1985GI02 J.Phys.(London) G11, 85 (1985) Combined Analysis of Pionic Atoms and Elastic Scattering of Alpha Particles ATOMIC PHYSICS, Mesic-Atoms 40,42,44,48Ca; analyzed pionic atom strong interaction shifts, widths data. 40,42,44,48Ca deduced neutron density radial moments. Elastic α-scattering data input. NUCLEAR REACTIONS 40,42,44,48Ca(α, α), E=104 MeV; analyzed σ(θ). 40,42,44,48Ca deduced neutron density radial moments. Pionic atom data input.
doi: 10.1088/0305-4616/11/1/013
1985MI05 Nucl.Phys. A435, 621 (1985) S.Micek, Z.Majka, H.Rebel, H.J.Gils, H.Klewe-Nebenius The Optical Potential for 6Li - 6Li Elastic Scattering at 156 MeV NUCLEAR REACTIONS 6Li(6Li, 6Li), E=156 MeV; measured σ(E(6Li), θ), σ(θ); deduced optical potentials. Semi-microscopic double folding cluster model.
doi: 10.1016/0375-9474(85)90480-4
1985SA36 Z.Phys. A322, 627 (1985) Y.Sakuragi, M.Kamimura, S.Micek, H.Rebel, H.J.Gils 6Li Break-Up Effect on Elastic and Inelastic Scattering of 6Li + 6Li at 156 MeV NUCLEAR REACTIONS 6Li(6Li, 6Li), (6Li, 6Li'), E=156 MeV; measured σ(θ). 6Li deduced breakup channel coupling role. Coupled, discretized continuum channels model.
doi: 10.1007/BF01415144
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
1984GI03 Phys.Rev. C29, 1295 (1984) Isotopic and Isotonic Differences between α Particle Optical Potentials and Nuclear Densities of 1f7/2 Nuclei NUCLEAR REACTIONS 40,42,43,44,48Ca, 50Ti, 51V, 52Cr(α, α), E=104 MeV; analyzed σ(θ); deduced isotopic, isotonic differences of optical potentials and nuclear matter densities. Fourier-Bessel potential, folding model analysis.
doi: 10.1103/PhysRevC.29.1295
1984GI06 Z.Phys. A317, 65 (1984) Local Density Approximation in Effective Density-Dependent αN-Interactions NUCLEAR REACTIONS 42,44,48Ca(α, α), E=104 MeV; 40Ca(α, α), E=104, 140 MeV; analyzed elastic scattering data; deduced potential parameters, local density approximation form. Folding model, effective density-dependent α-nucleon interactions.
doi: 10.1007/BF01420449
1983CO02 J.Phys.(London) G9, 177 (1983) V.Corcalciuc, H.Rebel, R.Pesl, H.J.Gils Isoscalar Octupole Transition Rates in 50Ti, 52Cr and 208Pb from Model-Independent Analyses of 104 MeV α-Particle Scattering NUCLEAR REACTIONS 50Ti, 52Cr, 208Pb(α, α), (α, α'), E=104 MeV; analyzed σ(θ). 50Ti, 52Cr, 208Pb deduced volume integrals, rms, transition radii, T=0 octupole transition strength. Model independent analysis.
doi: 10.1088/0305-4616/9/2/010
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
1982CO19 Nucl.Phys. A388, 173 (1982) J.Cook, H.J.Gils, H.Rebel, Z.Majka, H.Klewe-Nebenius Optical Model Studies of 6Li Elastic Scattering at 156 MeV NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 208Pb(6Li, 6Li), E=156 MeV; analyzed σ(θ); deduced potential form dependence. Phenomenological optical potential.
doi: 10.1016/0375-9474(82)90514-0
1982FR06 Phys.Rev. C25, 1551 (1982) Comparison between Radial Sensitivity of Different Strongly Interacting Probes NUCLEAR REACTIONS 48Ca(α, α), E=104 MeV; 48Ca(p, p), E=1 GeV; 48Ca(π+, π+), (π-, π-), E=50, 130 MeV; analyzed σ(θ). 48Ca deduced neutron density radial dependence, rms radii. Optical model, Fourier-Bessel method. ATOMIC PHYSICS, Mesic-Atoms 48Ca; calculated strong interaction shifts, widths; deduced surface effects. Optical model, Fourier-Bessel method.
doi: 10.1103/PhysRevC.25.1551
1982MA21 Phys.Rev. C25, 2996 (1982) Cluster Folding Model for 12C(6Li, 6Li) Scattering at 156 MeV NUCLEAR REACTIONS 12C(6Li, 6Li), E=156 MeV; calculated σ(θ). Double-folding cluster model potential.
doi: 10.1103/PhysRevC.25.2996
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
1981FR10 Nucl.Phys. A363, 137 (1981) E.Friedman, H.J.Gils, H.Rebel, R.Pesl The Dependence on Energy and Mass Number of the α-Particle Optical Potential: Support for the folding model approach NUCLEAR REACTIONS 40,42,44,48Ca, 50Ti, 52Cr, 90Zr(α, α), E=104 MeV; 40Ca, 46,48,50Ti, 58Ni, 90Zr, 208Pb(α, α), E=140 MeV; 58,60,62,64Ni(α, α), E=173 MeV; analyzed σ(θ); deduced mass, energy dependence of rms radius of optical potential components. Fourier-Bessel description.
doi: 10.1016/0375-9474(81)90458-9
1981RE09 Nucl.Phys. A368, 61 (1981) H.Rebel, R.Pesl, H.J.Gils, E.Friedman Method for Analysis of Inelastic α-Particle Scattering NUCLEAR REACTIONS 50Ti, 52Cr(α, α'), E=104 MeV; calculated σ(θ). Fourier-Bessel method.
doi: 10.1016/0375-9474(81)90730-2
1980CO13 Rev.Roum.Phys. 25, 471 (1980) V.Corcalciuc, R.Dumitrescu, A.Ciocanel, H.J.Gils, H.Rebel, W.Stach, S.Zagromski On the Fine Structure of Inelastic Scattering Angular Distributions NUCLEAR REACTIONS 68Zn(3He, 3He), (3He, 3He'), E=29 MeV; measured σ(θ); deduced no fine structure.
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
1980MA35 Acta Phys.Pol. B11, 227 (1980) Saturation Effect and Determination of Nuclear Matter Density Distribution from Optical Potential NUCLEAR REACTIONS 48,40Ca(α, α), E=104 MeV; calculated σ(θ); deduced real α-nucleus potential radii. 40,48Ca deduced comparative nuclear matter distributions. Double folding model, density-dependent nucleon-nucleon interaction.
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
1978FR22 Phys.Rev.Lett. 41, 1220 (1978) E.Friedman, H.J.Gils, H.Rebel, Z.Majka 48Ca-40Ca Radius Difference from Elastic Scattering of 104-MeV α Particles NUCLEAR REACTIONS 40,48Ca(α, α), E=104 MeV; measured σ(θ). 40,48Ca deduced nuclear matter rms radius difference.
doi: 10.1103/PhysRevLett.41.1220
1978MA40 Z.Phys. A288, 139 (1978) 104 MeV Alpha Particle and 156 MeV 6Li Scattering and the Validity of Refined Folding Model Approaches for Light Complex Projectile Scattering NUCLEAR REACTIONS 40,48Ca(α, α), E=104 MeV; 40,48Ca(6Li, 6Li), E=156 MeV; calculated real parts of optical potential.
doi: 10.1007/BF01408643
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
1976GI05 Phys.Rev. C13, 2159 (1976) Differences between Neutron and Proton Density rms Radii of 204,206,208Pb Determined by 104 MeV α Particle Scattering NUCLEAR REACTIONS 204,206,208Pb(α, α), E=104 MeV; measured σ(θ); deduced neutron density rms radii. Microscopic optical model analysis. Enriched targets.
doi: 10.1103/PhysRevC.13.2159
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
1976GI12 Nuovo Cim. 36A, 258 (1976) Experimental Studies of Neutron Collectivities by α-Particle Scattering and Some Implications for Giant-Resonance Excitations NUCLEAR REACTIONS 208Pb(α, α), (α, α'), E=104 MeV; analyzed data; calculated σ for GDR in 208Pb.
doi: 10.1007/BF02724579
1975FL07 Z.Phys. A272, 219 (1975) D.Flothmann, H.J.Gils, W.Wiesner, R.Lohken Spectral Shape of the (7/2- → 5/2+)-Transition in the β-Decay of 139Ba RADIOACTIVITY 139Ba, 90Y; measured βγ-coin, β shape spectrum; deduced Eβ max.
doi: 10.1007/BF01408151
1975GI04 J.Phys.(London) G1, 344 (1975) H.J.Gils, H.Rebel, G.Nowicki, A.Ciocanel, D.Hartmann, H.Klewe-Nebenius, K.Wisshak Deformation of 56Fe from 104 MeV α-Particle Scattering NUCLEAR REACTIONS 56Fe(α, α'), (α, α), E=104 MeV; analyzed σ(Eα', θ). 56Fe levels deduced β, B(E2), quadrupole moment.
doi: 10.1088/0305-4616/1/3/009
1975GI10 Z.Phys. A274, 259 (1975) Isoscalar Transition Rates from Folding Model Analysis of (α, α') Scattering NUCLEAR REACTIONS 20Ne, 56Fe, 58,60Ni, 90Zr, 116Sn(α, α'), E=104 MeV; analyzed σ(Eα', θ). 20Ne, 56Fe, 58,60Ni, 90Zr, 116Sn levels deduced B(λ).
doi: 10.1007/BF01437738
1974GI10 Rev.Roum.Phys. 19, 761 (1974) Evidence for Prolate Deformation of 56Fe from 104 MeV α-Particle Scattering NUCLEAR REACTIONS 56Fe(α, α), (α, α'), E=104 MeV; measured σ(θ), σ(Eα', θ). 56Fe levels deduced quadrupole moment, β, B(E2), B(E4).
1974RE04 Nucl.Phys. A225, 457 (1974) H.Rebel, G.W.Schweimer, D.Habs, H.J.Gils Generalized Collective Model and α-Particle Scattering on 56Fe and 48Ti NUCLEAR REACTIONS 48Ti, 56Fe(α, α), (α, α'), E=104 MeV; calculated σ(θ), B(E2).
doi: 10.1016/0375-9474(74)90353-4
1972FL07 Nucl.Instrum.Methods 102, 237 (1972) D.Flothmann, H.J.Gils, R.Lohken, W.Wiesner Reproduction of Monoenergetic Electron Lines in a 4π-Si(Li)-β-Spectrometer Using a Coincidence Method RADIOACTIVITY 113mIn, 137mBa; measured (K X-ray)ce-coin.
doi: 10.1016/0029-554X(72)90719-7
1972GI17 Nucl.Instrum.Methods 105, 179 (1972) H.J.Gils, D.Flothmann, R.Lohken, W.Wiesner A 4π β-γ-Coincidence Spectrometer Using Si(Li) and NaI(Tl) Detectors RADIOACTIVITY 22,24Na; measured βγ-coin; deduced Q, shape factors. NaI(Tl), Si(Li) detectors.
doi: 10.1016/0029-554X(72)90556-3
1972WI18 Nucl.Phys. A191, 166 (1972) W.Wiesner, D.Flothmann, H.J.Gils, R.Lohken, H.Rebel Spectral Shape and Nuclear Matrix Elements in the β-Decay of 206Tl RADIOACTIVITY 206Tl[from 205Tl(d, p)]; measured T1/2, Eβ, spectrum shape; calculated matrix elements. 4π Si(Li) spectrometer(5mm detectors), isotope-separated sources.
doi: 10.1016/0375-9474(72)90600-8
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