NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = H.Rebel Found 138 matches. Showing 1 to 100. [Next]2012RE03 Rom.J.Phys. 57, 472 (2012) Information about High-Energy Hadronic Interaction Processes from Extensive Air Shower Observations
2003BR20 Nucl.Phys. A721, 1044c (2003) I.M.Brancus, J.Wentz, B.Mitrica, H.Rebel, M.Petcu, H.Bozdog, H.J.Mathes, A.F.Badea, A.Bercuci, C.Aiftimiei, M.Duma, A.Meli, G.Toma, B.Vulpescu The East-West effect of the muon charged ratio at energies relevant to the atmospheric neutrino anomaly
doi: 10.1016/S0375-9474(03)01281-8
2001VU01 J.Phys.(London) G27, 977 (2001) B.Vulpescu, J.Wentz, I.M.Brancus, H.Rebel, A.F.Badea, H.Bozdog, H.J.Mathes, M.Petcu, M.Duma The Charge Ratio of Atmospheric Muons below 1.0 GeV c-1 by Measuring the Lifetime of Muonic Atoms in Aluminium ATOMIC PHYSICS, Mesic-atoms 27Al; measured muonic atoms decay rates; deduced charge ratio of atmospheric neutrinos.
doi: 10.1088/0954-3899/27/5/303
2000RE09 Nucl.Phys. A663-664, 847c (2000) H.Rebel, for the KASCADE Collaboration How to Infer Mass Composition of Cosmic Rays from Extensive Air Shower Observations
doi: 10.1016/S0375-9474(99)00729-0
2000SC11 Eur.Phys.J. A 7, 367 (2000) K.Schwarz, C.Samanta, M.Fujiwara, H.Rebel, R.De Leo, N.Matsuoka, H.Utsunomiya, H.Akimune, I.Daito, H.Fujimura, F.Ihara, K.Ishibashi, Y.Maeda, T.Yamanaka, H.Yoshida, A.Okihana, T.Yoshimura, P.K.J.van Aarle, W.A.T.Uijen, M.Ito, Y.Sakuragi Reaction Mechanism of 6Li Scattering at 600 MeV NUCLEAR REACTIONS 12C, 58Ni, 90Zr, 208Pb(6Li, 6Li), (6Li, dα), E= 600 MeV; measured elastic and breakup σ(θ), particle spectra. Comparison with theoretical calculations.
doi: 10.1007/PL00013619
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
1998SC21 Phys.Rep. 294, 167 (1998) H.Schatz, A.Aprahamian, J.Gorres, M.Wiescher, T.Rauscher, J.F.Rembges, F.-K.Thielemann, B.Pfeiffer, P.Moller, K.-L.Kratz, H.Herndl, B.A.Brown, H.Rebel rp-Process Nucleosynthesis at Extreme Temperature and Density Conditions
doi: 10.1016/S0370-1573(97)00048-3
1997GR11 Nucl.Phys. A621, 603c (1997) U.Greife, C.Arpesella, E.Bellotti, K.Brand, C.Broggini, L.Campajola, P.Corvisiero, A.D'Onofrio, G.Fiorentini, A.Fubini, G.Gervino, L.Gialanella, C.Gustavino, E.Huttel, M.Junker, R.W.Kavanagh, R.Kubat, J.Lambert, G.Oliviero, P.Prati, H.Rebel, V.Roca, W.S.Rodney, C.Rolfs, M.Romano, M.Romoli, S.Schmidt, W.H.Schulte, F.Strieder, F.Terrasi, H.P.Trautvetter, D.Zahnow, S.Zavatarelli Further Direct Approaches to the Nuclear Reactions in the Sun
doi: 10.1016/S0375-9474(97)00312-6
1996CA43 Z.Phys. A356, 107 (1996) L.Campajola, L.Gialanella, K.Brand, A.D'Onofrio, U.Greife, E.Huttel, R.Kubat, G.Oliviero, H.Rebel, V.Roca, C.Rolfs, M.Romano, M.Romoli, S.Schmidt, W.H.Schulte, F.Strieder, F.Terrasi, H.-P.Trautvetter, D.Zahnow Production of an 8.0 MeV 7Be Ion Beam at the Naples TTT-3 Accelerator NUCLEAR REACTIONS 1H(7Be, γ), E=8 MeV; measured residual nuclei production. Radioactive beam from 7Li(p, n) reaction.
doi: 10.1007/s002180050154
1996RE16 Acta Phys.Pol. B27, 231 (1996) Coulomb Dissociation Experiments of Astrophysical Significance NUCLEAR REACTIONS 3He, 7Be, 6,7Li, 12,14C, 16,15O, 14N(α, γ), 9,7Be, 6Li, 10,11B, 11,12C, 16O, 13N, 20Ne, 31S(p, γ), 4He(d, γ), (t, γ), 12,14C(n, γ), E not given; compiled, reviewed capture reactions accessible to fast projectile Coulomb dissociation studies.
1996SI13 Z.Phys. A355, 397 (1996) T.Sinha, R.Kanungo, C.Samanta, S.Ghosh, P.Basu, H.Rebel Coupling Effects of Resonant and Discretized Non-Resonant Continuum States in 4He + 6Li Scattering at 10 MeV/A NUCLEAR REACTIONS 6Li(α, α'), (α, α), E=40 MeV; analyzed σ(θ); deduced nonresonant continuum states coupling strengths related features. Coupled-channels approach.
doi: 10.1007/s002180050128
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
1995KA07 Z.Phys. A351, 9 (1995) R.Kanungo, M.Lahiri, C.Samanta, H.Rebel Continuum-Continuum Coupling with Discretized 6Li → α + d Breakup Continuum Data NUCLEAR REACTIONS 6Li(α, α'), (α, α), E=50 MeV; 6Li(p, p), (p, p'), E=65 MeV; analyzed σ(θ); deduced minimal continuum-continuum coupling.
doi: 10.1007/BF01292779
1995KA43 Int.J.Mod.Phys. E4, 827 (1995) R.Kanungo, M.Lahiri, C.Samanta, H.Rebel Studies of Continuum Coupling Effects in 6Li(α, α') and 6Li(p, p') Excitation NUCLEAR REACTIONS 6Li(p, p'), E=65 MeV; 6Li(α, α'), E=50 MeV; analyzed σ(θ); deduced marginal coupling due to multi-step processes. Realistic coupled-channels approach.
doi: 10.1142/S0218301395000298
1994BB15 J.Phys.(London) G20, 1 (1994) Coulomb Dissociation Studies as a Tool of Nuclear Astrophysics
doi: 10.1088/0954-3899/20/1/005
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.
1992RI04 Z.Phys. A342, 487 (1992) J.Rink, B.Gorski, W.Kalber, G.Meisel, H.-J.Mielke, H.Rebel, M.Schubert Optical Isotope Shift of 172Hf(T1/2 = 1.87 a) NUCLEAR MOMENTS 176,177,178,178m,180Hf; measured optical isotope shifts. RADIOACTIVITY 172Hf(EC); measured optical isotope shifts. 172,178Hf deduced rms charge radii.
doi: 10.1007/BF01294960
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
1991KO32 Phys.Rev. A44, R1442 (1991) D.Kowalewska, K.Bekk, S.Goring, A.Hanser, W.Kalber, G.Meisel, H.Rebel Isotope Shifts and Hyperfine Structure in Polonium Isotopes by Atomic-Beam Laser Spectroscopy RADIOACTIVITY 200,202,204,205,206,207,208,209,210Po; measured hfs, isotope shifts; deduced rms charge radii changes, relative variation with respect to neighboring elements. Laser-induced fluorescence spectroscopy.
doi: 10.1103/PhysRevA.44.R1442
1990BR20 Phys.Rev. C42, 2157 (1990) I.M.Brancus, H.Rebel, J.Wentz, V.Corcalciuc Extended Sum-Rule Model View of Light and Intermediate Mass Fragment Emission in Nuclear Reactions at Intermediate Energies NUCLEAR REACTIONS Ag(6Li, X), E=156 MeV; Ag(12C, X), E=576 MeV; Ag(3He, X), E=198.6 MeV; 58Ni, Ag(α, X), E=104 MeV; Ag(40Ar, X), E=336 MeV; calculated intermediate mass fragment emission σ vs charge. Ag(40Ar, X), E=336 MeV; calculated fragment production σ vs l for X=12B, 7Be, 5Li, 4He. Extended sum rule model.
doi: 10.1103/PhysRevC.42.2157
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
1990SR01 Nucl.Phys. A506, 346 (1990) D.K.Srivastava, H.Rebel, N.Heide A Prior-Form Distorted-Wave Born Approximation Analysis of the Elastic Breakup of 156 MeV 6Li Projectiles NUCLEAR REACTIONS 208Pb(6Li, dα), E=156 MeV; analyzed σ(θα, θd). Prior-form DWBA.
doi: 10.1016/0375-9474(90)90391-X
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
1989DE26 Z.Phys. D13, 181 (1989) J.Dembczynski, M.Elantkowska, K.Bekk, H.Rebel, M.Wilson Reanalysis of the Am I Level Spectrum and the Nuclear Quadrupole Moments of Am-Isotopes RADIOACTIVITY 241Am; analyzed hfs data; deduced hyperfine constants. 241Am deduced electric quadrupole moment.
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
1989GR13 Phys.Lett. 223B, 287 (1989) K.Grotowski, J.Ilnicki, T.Kozik, J.Lukasik, S.Micek, Z.Sosin, A.Wieloch, N.Heide, H.Jelitto, J.Kiener, H.Rebel, S.Zagromski, A.J.Cole Compound Nucleus Emission of Intermediate Mass Fragments in the 6Li + Ag Reaction at 156 MeV NUCLEAR REACTIONS 46Ti, Cu, Ag(6Li, X), E=156 MeV; measured σ vs fragment Z, σ(θ) vs fragment Z; deduced reaction mechanism.
doi: 10.1016/0370-2693(89)91603-1
1989HE17 Phys.Rev.Lett. 63, 601 (1989) N.Heide, D.K.Srivastava, H.Rebel Interference and Off-Shell Effects of Fragment Scattering in Elastic Breakup of Light Ions NUCLEAR REACTIONS 12C, 208Pb(6Li, dα), E=156 MeV; measured σ(θd, θα, Eα). 51V(3He, pd), E=90 MeV; analyzed σ(θp, θd, Ed). 118Sn(d, np), E=56 MeV; analyzed σ(θp, θn, En); deduced reaction mechanism. Prior form DWBA.
doi: 10.1103/PhysRevLett.63.601
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.
1989KA29 Z.Phys. A334, 103 (1989) W.Kalber, J.Rink, K.Bekk, W.Faubel, S.Goring, G.Meisel, H.Rebel, R.C.Thompson Nuclear Radii of Thorium Isotopes from Laser Spectroscopy of Stored Ions NUCLEAR MOMENTS 232Th; measured hfs, isotope shifts. 232,227,228,229,230Th deduced mean square charge radii change. Other data input. RADIOACTIVITY 227,228,229,230Th; measured hfs, isotope shifts. 232,227,228,229,230Th deduced mean square charge radii change. Other data input.
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.
1988BE30 Z.Phys. A330, 235 (1988) K.Bekk, S.Goring, W.Kalber, G.Meisel, H.Rebel, A.Ali Sameh Determination of the 242mAm Nuclear Moments RADIOACTIVITY 242mAm; measured hfs; deduced μ, electric quadrupole moment. Atomic beam, laser spectroscopy.
1988SR01 Phys.Lett. 206B, 391 (1988) D.K.Srivastava, D.N.Basu, H.Rebel Direct and Sequential Coulomb Break-Up of 7Li NUCLEAR REACTIONS 120Sn(7Li, 7Li'), E=70 MeV; calculated pure Coulomb breakup σ(θ). 208Pb(7Be, 3Heα), (7Be, tα), E=40-300 MeV; calculated breakup σ(E).
doi: 10.1016/0370-2693(88)91597-3
1988SR02 Nucl.Phys. A485, 221 (1988) D.K.Srivastava, D.N.Basu, H.Rebel The Dynamic Polarization Potential from Coulomb Dissociation of Deuterons and 3He NUCLEAR REACTIONS, ICPND 208Pb(d, np), (3He, pd), E ≈ 10-250 MeV; calculated Coulomb dissociation σ(E). Dynamic polarization. NUCLEAR STRUCTURE 3He, 2H; calculated B(E2) per unit energy following Coulomb dissociation. Dynamic polarization.
doi: 10.1016/0375-9474(88)90099-1
1988SR03 Phys.Rev. C38, 2148 (1988) D.K.Srivastava, D.N.Basu, H.Rebel Features of Direct and Sequential Coulomb Breakup of 6Li Ions NUCLEAR REACTIONS 208Pb(6Li, dα), E=30-156 MeV; calculated Coulomb dissociation σ(E); deduced breakup mechanism, relation to astrophysical S-factor. NUCLEAR STRUCTURE 6Li; calculated breakup transition B(E2).
doi: 10.1103/PhysRevC.38.2148
1987AN02 Z.Phys. A326, 493 (1987) M.Anselment, K.Bekk, S.Chongkum, S.Goring, A.Hanser, H.Hoeffgen, W.Kalber, G.Meisel, H.Rebel Charge Radii and Moments of Strontium Nuclei by Laser Spectroscopy RADIOACTIVITY 80,81,82,83,85Sr(EC); 85m,87mSr(IT); 89,90Sr(β-); measured hfs, isotope shifts. 80,81,82,83,85,85m,87m,88,89,90Sr deduced μ, electric quadrupole moments, rms charge radii. NUCLEAR MOMENTS 84,86,87,88Sr; measured hfs, isotope shifts. 84,86,87,88Sr deduced μ, electric quadrupole moments, mean square charge radii.
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
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.
1987ME22 Hyperfine Interactions 38, 723 (1987) G.Meisel, K.Bekk, H.Rebel, G.Schatz Atomic Beam, Optogalvanic and Stored Ion Spectroscopy for Radioactive Isotopes NUCLEAR MOMENTS 204,206,208,207Pb; measured hfs, isotope shifts. Laser induced resonance absorption. NUCLEAR STRUCTURE 241,242m,243Am; measured optical isotope shifts. Laser induced resonances absorption.
doi: 10.1007/BF02394871
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.
1986AN06 Nucl.Phys. A451, 471 (1986) M.Anselment, W.Faubel, S.Goring, A.Hanser, G.Meisel, H.Rebel, G.Schatz The Odd-Even Staggering of the Nuclear Charge Radii of Pb Isotopes RADIOACTIVITY 196,197,197m,211,214Pb; measured hfs, isotope shift; deduced hyperfine constants. 196,197,197m,198,199,200,201,202,202m,203,204,205,206,207,208,209,210,211,212,214Pb deduced nuclear charge radii, nuclear, odd-even staggering parameters, μ, quadrupole moment. Laser spectroscopic techniques, other data input.
doi: 10.1016/0375-9474(86)90071-0
1986AN24 Phys.Rev. C34, 1052 (1986) M.Anselment, K.Bekk, A.Hanser, H.Hoeffgen, G.Meisel, S.Goring, H.Rebel, G.Schatz Charge Radii and Moments of Tin Nuclei by Laser Spectroscopy NUCLEAR MOMENTS 112,114,115,116,117,118,119,120,122,124Sn; measured isotope shift, hfs; deduced rms charge radius, μ, electric quadrupole moments. Laser spectroscopy. RADIOACTIVITY 117m,110,111,113,121,121m,123,125Sn; measured isotope shift, hfs; deduced rms charge radius differences, magnetic dipole, electric quadrupole moments. Laser spectroscopy.
doi: 10.1103/PhysRevC.34.1052
1986AN39 Z.Phys. D3, 421 (1986) M.Anselment, S.Chongkum, K.Bekk, S.Goring, A.Hanser, G.Meisel, H.Rebel Isotope Shift of a Series of Sr Isotopes RADIOACTIVITY 80,81,82,83,85,89,90Sr; measured isotope shift. NUCLEAR MOMENTS 84,86Sr; measured isotope shift.
doi: 10.1007/BF01437201
1986BA50 Nucl.Phys. A458, 188 (1986) G.Baur, C.A.Bertulani, H.Rebel Coulomb Dissociation as a Source of Information on Radiative Capture Processes of Astrophysical Interest NUCLEAR REACTIONS 208Pb(7Be, 3Heα), E=30 MeV/nucleon; 208Pb(16O, 12Cα), E=1000 MeV; calculated virtual photon spectra and kinematical loci; 7Be(γ, α), E ≥ 1.658 MeV; 16O(γ, α), E ≥ 8.162 MeV; calculated σ. Coulomb dissociation mechanism.
doi: 10.1016/0375-9474(86)90290-3
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
1986SR02 J.Phys.(London) G12, 717 (1986) Resonant and Non-Resonant Coulomb Break-Up of 6Li NUCLEAR REACTIONS 208Pb(6Li, dα), E=156 MeV; calculated σ(θα, θd, Eα). 6Li deduced resonant, nonresonant breakup in Coulomb field.
doi: 10.1088/0305-4616/12/8/008
1985AL24 Nucl.Phys. A445, 477 (1985) J.Albinski, A.Budzanowski, H.Dabrowski, Z.Rogalska, S.Wiktor, H.Rebel, D.K.Srivastava, C.Alderliesten, J.Bojowald, W.Oelert, C.Mayer-Boricke, P.Turek α-Particle Scattering from Ni Isotopes at E(α) = 172.5 MeV NUCLEAR REACTIONS 58,60,62,64Ni(α, α'), E=172.5 MeV; measured σ(θ); deduced optical potentials. 58,60,62,64Ni deduced rms radii differences, dynamic deformation parameters, isoscalar B(λ). Coupled-channels analyses. Enriched targets.
doi: 10.1016/0375-9474(85)90453-1
1985FU08 Phys.Rev. C32, 418 (1985) K.Fuchs, W.Eyrich, A.Hofmann, B.Muhldorfer, U.Scheib, H.Schlosser, H.Rebel Neutron Decay of the Isoscalar Giant Resonance Region in 90Zr NUCLEAR REACTIONS 90Zr(α, α'n), E=104 MeV; measured σ(Eα'), σ(θα, θn). 90Zr deduced isoscalar giant resonances, multipolarity, decay characteristics.
doi: 10.1103/PhysRevC.32.418
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
1984DE06 Z.Phys. A315, 137 (1984) Fine- and Hyperfine Structure Analysis of the Odd Configurations in the Lead Atom ATOMIC PHYSICS Pb; analyzed fine structure, hfs data; deduced Slater integrals, spin-orbit, effective hfs one-electron parameters. NUCLEAR MOMENTS Pb; analyzed hfs data. 199,201,202m,203,205,209Pb deduced quadrupole moment.
1984EY01 Phys.Rev. C29, 418 (1984) W.Eyrich, K.Fuchs, A.Hofmann, U.Scheib, H.Steuer, H.Rebel Direct Decay Component of the Giant-Monopole-Resonance Region in 208Pb NUCLEAR REACTIONS 208Pb(α, α'n), E=104 MeV; measured σ(Eα'), σ(θα, θn); deduced preequilibrium neutron decay. 208Pb deduced giant monopole resonance decay characteristics.
doi: 10.1103/PhysRevC.29.418
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
1984SR01 Z.Phys. A316, 225 (1984) The Density Dependence of the Effective Alpha-Nucleon Force and Isoscalar Transition Rates of Nuclei NUCLEAR REACTIONS 20Ne, 24Mg, 28Si, 32S, 40Ar, 42Ca, 48Ti, 52Cr, 56Fe, 60Ni, 66Zn, 72Ge, 76Se, 88Sr, 90Zr, 96Mo, 100Ru, 106Pd, 110Cd, 116Sn, 124Te, 136Ba, 144Nd, 148Sm, 194Pt, 200Hg, 206Pb(α, α'), E not given; calculated effective α-nucleon force density dependence. 20Ne, 24Mg, 28Si, 32S, 40Ar, 42Ca, 48Ti, 52Cr, 56Fe, 60Ni, 66Zn, 72Ge, 76Se, 88Sr, 90Zr, 96Mo, 100Ru, 106Pd, 110Cd, 116Sn, 124Te, 136Ba, 144Nd, 148Sm, 194Pt, 200Hg, 206Pb deduced isoscalar transition rate corrections. Folding procedures.
doi: 10.1007/BF01412267
1984SR02 J.Phys.(London) G10, L127 (1984) Evidence for a Dynamic Density Dependence of the Alpha-Nucleon Force in Inelastic Scattering of Alpha Particles NUCLEAR REACTIONS 50Ti, 52Cr(α, α), (α, α'), E=104 MeV; analyzed σ(θ); deduced α-nucleon force dynamic density dependence. Deformed folding model.
doi: 10.1088/0305-4616/10/6/004
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
1983FA11 Nucl.Instrum.Methods 213, 277 (1983) H.R.Faust, H.Klewe-Nebenius, H.Rebel, K.Wisshak Determination of the Multipolarity of Prompt Electromagnetic Transitions from Angular Distributions of Conversion Electrons Part II: Spectrometer and Measurements NUCLEAR REACTIONS 169Tm, 192Os(d, 5n), E=52 MeV; measured I(ce), ce(θ). 166Yb, 189Ir deduced rotational band transition angular distribution coefficients. Mini-orange spectrometer, magnetic filter system.
doi: 10.1016/0167-5087(83)90420-9
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
1983TH03 J.Phys.(London) G9, 443 (1983) R.C.Thompson, M.Anselment, K.Bekk, S.Goring, A.Hanser, G.Meisel, H.Rebel, G.Schatz, B.A.Brown High-Resolution Measurements of Isotope Shifts and Hyperfine Structure in Stable and Radioactive Lead Isotopes RADIOACTIVITY 210Pb; 212Pb [from 232Th decay]; 205Pb [from 204Pb(n, γ)]; 209Pb [from 208Pb(d, p)]; 198,199,200,202Pb [from Hg(α, xn), E=104 MeV]; 201,202m,203Pb [from Tl(d, xn), E=38, 48 MeV]; measured hfs, isotope shifts. 201,202m,205,209Pb deduced μ, quadrupole moment, rms charge radii. 199Pb level deduced J, π, μ, quadrupole moment, rms charge radius. 198,210,212Pb deduced rms charge radius. Droplet model, Skyrme interactions. NUCLEAR MOMENTS 204,206,207Pb; measured hfs, isotope shifts; deduced rms charge radii. Droplet model, Skyrme interactions.
doi: 10.1088/0305-4616/9/4/010
1982AN15 Phys.Rev. C26, 2194 (1982) A.Andl, K.Bekk, S.Goring, A.Hanser, G.Nowicki, H.Rebel, G.Schatz, R.C.Thompson Isotope Shifts and Hyperfine Structure of the 4s2 1S0-4s4p 1P1 Transition in Calcium Isotopes NUCLEAR MOMENTS 40,42,43,44,46,48Ca, 41,45,47Ca [from 40,44,46Ca(n, γ), E=thermal]; measured hfs, isotope shifts. 41,45,47Ca deduced hyperfine constants, rms charge radii differences, μ. 43Ca deduced hyperfine constants, rms charge radii differences. 40,42,44,46,48Ca deduced rms charge radii differences. Laser spectroscopy, resonance fluorescence technique.
doi: 10.1103/PhysRevC.26.2194
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
1981EY02 Phys.Rev. C24, 2720 (1981) W.Eyrich, H.Hassold, A.Hofmann, B.Muhldorfer, U.Scheib, H.Rebel Search for E0 Strength in the Giant Resonance Region of 12C NUCLEAR REACTIONS 12C(α, α'), E=104 MeV; measured σ(Eα), σ(θ). 12C deduced no monopole resonance.
doi: 10.1103/PhysRevC.24.2720
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
1981ST25 Phys.Rev.Lett. 47, 1702 (1981) H.Steuer, W.Eyrich, A.Hofmann, H.Ortner, U.Scheib, R.Stamminger, D.Steuer, H.Rebel Neutron Decay of the Giant Quadrupole Resonance Region in 208Pb NUCLEAR REACTIONS 208Pb(α, α'n), E=104 MeV; measured nα-coin, Eα, En. 208Pb deduced GQR branching ratio. 207Pb levels deduced populating γ-multipolarity.
doi: 10.1103/PhysRevLett.47.1702
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
1979BE25 Z.Phys. A291, 219 (1979) K.Bekk, A.Andl, S.Goring, A.Hanser, G.Nowicki, H.Rebel, G.Schatz Laserspectroscopic Studies of Collective Properties of Neutron Deficient Ba Nuclei NUCLEAR MOMENTS 126,129m,129,135mBa; measured optical isotope shift, hfs. 126,129m,129,135mBa deduced differences of rms charge radii, μ, quadrupole moment. Laser spectroscopy. Quasiparticle-plus-triaxial rotor, droplet model.
doi: 10.1007/BF01409187
1979EY02 Phys.Rev.Lett. 43, 1369 (1979) W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel Decay of the Isoscalar Giant Resonances in 208Pb NUCLEAR REACTIONS 208Pb(α, α'), E=104 MeV; measured α'γ(θ). 208Pb deduced T=0, GQR, fine structure following n decay.
doi: 10.1103/PhysRevLett.43.1369
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
1979RO09 Phys.Lett. 88B, 51 (1979) H.Rost, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler, H.Rebel A Study of the Giant Resonance Region of 40Ca by Inelastic Scattering Of 104 MeV α-Particles NUCLEAR REACTIONS 40Ca(α, α'), E=104 MeV; measured σ(θ). 40Ca resonances deduced L, β2, energy-weighted sum rule strengths for E2. DWBA analysis.
doi: 10.1016/0370-2693(79)90111-4
1979RU08 Z.Phys. A293, 287 (1979) P.Rullhusen, F.Smend, M.Schumacher, A.Hanser, H.Rebel Coulomb Correction to Delbruck Scattering Investigated at Z = 94 NUCLEAR REACTIONS 239Pu(γ, γ), E=2.754 MeV; measured σ(θ); deduced higher-order Coulomb correction terms. Delbruck, nuclear resonance scattering analysis.
doi: 10.1007/BF01435270
1978EY02 Fizika, Suppl. 10, 45 (1978) W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel The Deformation of 26Mg from Particle-Gamma Angular Correlations NUCLEAR REACTIONS 24,26Mg, 28Si(α, α'), E=104 MeV; measured αγ(θ). 24,26Mg, 28Si level deduced β. Coupled-channels analysis.
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
1978NO09 Phys.Rev. C18, 2369 (1978) G.Nowicki, K.Bekk, S.Goring, A.Hanser, H.Rebel, G.Schatz Nuclear Charge Radii and Nuclear Moments of Neutron Deficient Ba Isotopes from High Resolution Laser Spectroscopy NUCLEAR MOMENTS 128,131,133Ba; measured isotope shift, hfs, J, nuclear charge radii. Laser spectroscopy.
doi: 10.1103/PhysRevC.18.2369
1977EY03 Nucl.Phys. A287, 119 (1977) W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel Alpha-Gamma Angular Correlations in the Reaction 24Mg(α, α1γ) at E = 104 MeV NUCLEAR REACTIONS 24Mg(α, α'γ), E=104 MeV; measured in-plane α'γ(θ). 24Mg deduced sign of the quadrupole deformation parameter. Coupled channels analyses, enriched target.
doi: 10.1016/0375-9474(77)90567-X
1977FE11 Phys.Lett. 69B, 407 (1977) W.Feix, W.Wilcke, T.W.Elze, H.Rebel, J.R.Huizenga, R.C.Thompson, R.M.Dreizler Study of Nuclear-Coulomb Interference Effects in Inelastic Deuteron Scattering on 238U NUCLEAR REACTIONS 238U(d, d), (d, d'), E=17 MeV; measured σ(θ). 238U deduced β.
doi: 10.1016/0370-2693(77)90831-0
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
1977NO04 Phys.Rev.Lett. 39, 332 (1977) G.Nowicki, K.Bekk, S.Goring, H.Hanser, H.Rebel, G.Schatz Nuclear Radii and Magnetic Moments of 128,131Ba from High-Resolution Laser Spectroscopy NUCLEAR MOMENTS 128,131Ba; measured isotope shift, hfs. 128,130,131Ba deduced differences of mean-square charge radii. 131Ba deduced μ. Doppler-free laser spectroscopy.
doi: 10.1103/PhysRevLett.39.332
1976EY02 Phys.Lett. 63B, 406 (1976) W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel Alpha-Gamma Angular Correlation Measurements as a Sensitive Method Determining the Sign of the Nuclear Quadrupole Deformation NUCLEAR REACTIONS 24Mg(α, α'γ), E=104 MeV; measured γγ(θ). 24Mg levels deduced sign of β2.
doi: 10.1016/0370-2693(76)90381-6
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
1976RE04 Z.Phys. A277, 35 (1976) How to Extract Isoscalar Transition Rates from Alpha Particle Scattering Experiments NUCLEAR REACTIONS 16O(α, α'), E=146 MeV; analyzed method of determining isoscalar transition rates.
doi: 10.1007/BF01547499
Back to query form [Next] Note: The following list of authors and aliases matches the search parameter H.Rebel: , H.G.REBEL |