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2012RE03      Rom.J.Phys. 57, 472 (2012)

H.Rebel, O.Sima

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1725.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0245.


1996RE16      Acta Phys.Pol. B27, 231 (1996)

H.Rebel

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1994BB15      J.Phys.(London) G20, 1 (1994)

G.Baur, H.Rebel

Coulomb Dissociation Studies as a Tool of Nuclear Astrophysics

doi: 10.1088/0954-3899/20/1/005
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2209.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1530.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1537.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1530.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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1986SR02      J.Phys.(London) G12, 717 (1986)

D.K.Srivastava, H.Rebel

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
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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
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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
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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
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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
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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
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1984DE06      Z.Phys. A315, 137 (1984)

J.Dembczynski, H.Rebel

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
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1984GI03      Phys.Rev. C29, 1295 (1984)

H.J.Gils, H.Rebel, E.Friedman

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
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1984SR01      Z.Phys. A316, 225 (1984)

D.K.Srivastava, H.Rebel

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
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1984SR02      J.Phys.(London) G10, L127 (1984)

D.K.Srivastava, H.Rebel

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
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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
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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
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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
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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
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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
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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
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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
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1982FR06      Phys.Rev. C25, 1551 (1982)

E.Friedman, H.J.Gils, H.Rebel

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
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1982MA21      Phys.Rev. C25, 2996 (1982)

Z.Majka, H.J.Gils, H.Rebel

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
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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
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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
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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
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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
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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
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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
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1980MA35      Acta Phys.Pol. B11, 227 (1980)

Z.Majka, H.J.Gils, H.Rebel

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
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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
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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
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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
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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
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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
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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
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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
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1978MA40      Z.Phys. A288, 139 (1978)

Z.Majka, H.J.Gils, H.Rebel

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
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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
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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
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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
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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
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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
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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
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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
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1976GI05      Phys.Rev. C13, 2159 (1976)

H.J.Gils, H.Rebel

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
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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
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1976GI12      Nuovo Cim. 36A, 258 (1976)

H.J.Gils, H.Rebel, W.Knupfer

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
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1976RE04      Z.Phys. A277, 35 (1976)

H.Rebel

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
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Note: The following list of authors and aliases matches the search parameter H.Rebel: , H.G.REBEL