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NSR database version of May 10, 2024.

Search: Author = H.J.Gils

Found 57 matches.

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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


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


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


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


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


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


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
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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
Citations: PlumX Metrics


1987GI06      Nucl.Phys. A473, 111 (1987)

H.J.Gils

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
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.


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
Citations: PlumX Metrics


1985GI02      J.Phys.(London) G11, 85 (1985)

H.J.Gils, E.Friedman

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
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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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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
Citations: PlumX Metrics


1984GI06      Z.Phys. A317, 65 (1984)

H.J.Gils

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
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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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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2262.


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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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
Citations: PlumX Metrics


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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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0332.


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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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0114.


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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0332.


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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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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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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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1098.


1975GI10      Z.Phys. A274, 259 (1975)

H.J.Gils, H.Rebel

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
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1974GI10      Rev.Roum.Phys. 19, 761 (1974)

H.J.Gils, H.Rebel, A.Ciocanel

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
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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
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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
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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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