NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = F.Michel Found 44 matches. 2007MI46 Eur.Phys.J. Special Topics 150, 41 (2007) Unexpected transparency in the scattering of fragile 6Li and 6He Nuclei NUCLEAR REACTIONS 12,14C(6He, 2α), E=35 MeV; measured Eα, Iα, αα-coin. 14C; deduced level energies.
doi: 10.1140/epjst/e2007-00261-1
2005MI29 Phys.Rev. C 72, 054601 (2005) Airy minima in the scattering of weakly bound light heavy ions NUCLEAR REACTIONS 12C(6Li, 6Li), E=13-318 MeV; 12C(6Li, 6Li'), E=24, 30 MeV; 16O(6Li, 6Li), E=13-48 MeV; 12C(6He, 6He), E=18 MeV; analyzed σ(θ); deduced transparency, refractive features.
doi: 10.1103/PhysRevC.72.054601
2004MI12 Eur.Phys.J. A 19, 333 (2004) Evolution of Airy structure in 12C(12C, 12C)12C between 5 and 10 MeV/A NUCLEAR REACTIONS 12C(12C, 12C), E=70-130 MeV; calculated σ(θ), incomplete absorption features, properties of Airy minima. Global optical potential.
doi: 10.1140/epja/i2003-10133-0
2004MI33 Nucl.Phys. A738, 231 (2004) Airy structure in inelastic light heavy-ion scattering? NUCLEAR REACTIONS 40Ca(α, α), (α, α'), E=29-100 MeV; analyzed σ(θ), energy dependence of Airy minima.
doi: 10.1016/j.nuclphysa.2004.04.037
2004MI46 Phys.Rev. C 70, 044609 (2004) Airy structure in inelastic light-ion and light heavy-ion scattering NUCLEAR REACTIONS 40Ca(α, α), (α, α'), E=28-100 MeV; 16O(16O, 16O), (16O, 16O'), E=124 MeV; analyzed σ(θ), Airy structure; deduced phase rules between elastic and inelastic scattering.
doi: 10.1103/PhysRevC.70.044609
2002MI19 Yad.Fiz. 65, 706 (2002); Phys.Atomic Nuclei 65, 674 (2002) F.Michel, F.Brau, G.Reidemeister, S.Ohkubo Interpretation of Airy Minima in 16O + 16O and 16O + 12C Elastic Scattering in Terms of a Barrier-Wave/Internal-Wave Decomposition NUCLEAR REACTIONS 16O(16O, 16O), E=124 MeV; 12C(16O, 16O), E=132 MeV; calculated σ(θ), contribution of barrier-wave/internal-wave interference to Airy minima.
doi: 10.1134/1.1471272
2002MI39 Phys.Rev.Lett. 89, 152701 (2002) F.Michel, G.Reidemeister, S.Ohkubo Luneburg Lens Approach to Nuclear Rainbow Scattering NUCLEAR REACTIONS 12C(16O, 16O), E=132 MeV; analyzed σ(θ). 16O(16O, 16O), E=75 MeV; analyzed potential, trajectory features. Luneburg lens approach, differences between optical and nuclear mechanisms discussed.
doi: 10.1103/PhysRevLett.89.152701
2001MI06 Phys.Rev. C63, 034620 (2001) F.Michel, G.Reidemeister, S.Ohkubo Airy Structure in 16O + 16O Elastic Scattering between 5 and 10 MeV/nucleon NUCLEAR REACTIONS 16O(16O, 16O), E=75-145 MeV; 12C(16O, 16O), E=132 MeV; calculated σ(θ), barrier- and internal-wave components; deduced origin of Airy structure. Comparison with nearside/farside decomposition.
doi: 10.1103/PhysRevC.63.034620
2000MI06 Phys.Rev. C61, 041601 (2000) F.Michel, G.Reidemeister, S.Ohkubo Unexpected Transparency in Low Energy 90Zr(α, α0) Scattering and α-Cluster Structure in 94Mo NUCLEAR REACTIONS 90Zr(α, α), E=18-40 MeV; analyzed σ, σ(θ); deduced optical potential features. 94Mo deduced α-cluster structure.
doi: 10.1103/PhysRevC.61.041601
2000MI20 Phys.Rev.Lett. 85, 1823 (2000) F.Michel, F.Brau, G.Reidemeister, S.Ohkubo Barrier-Wave-Internal-Wave Interference and Airy Minima in 16O + 16O Elastic Scattering NUCLEAR REACTIONS 16O(16O, 16O), E=124 MeV; calculated σ(θ); deduced role of barrier-wave - internal-wave interference mechanism.
doi: 10.1103/PhysRevLett.85.1823
1998BR01 Phys.Rev. C57, 1386 (1998) F.Brau, F.Michel, G.Reidemeister Barrier and Internal Wave Contributions to the Quantum Probability Density and Flux in Light Heavy-Ion Elastic Scattering NUCLEAR REACTIONS 40,44Ca(α, α), E=29 MeV; calculated σ(θ), optical model wavefunctions; deduced anomalous large angle scattering mechanism.
doi: 10.1103/PhysRevC.57.1386
1998MI33 Prog.Theor.Phys.(Kyoto), Suppl. 132, 7 (1998) F.Michel, S.Ohkubo, G.Reidemeister Local Potential Approach to the Alpha-Nucleus Interaction and Alpha-Cluster Structure in Nuclei NUCLEAR REACTIONS 16O, 40Ca, 36Ar, 90Zr, 208Pb(α, α), E=18-146 MeV; analyzed σ(θ); deduced optical potential features. 20Ne, 44Ti, 40Ca, 94Mo, 212Po deduced α-cluster structure features.
doi: 10.1143/PTPS.132.7
1996MI07 Phys.Rev. C53, 3032 (1996) Pauli Forbidden States and the α + 14C Optical Potential NUCLEAR REACTIONS 14C(α, α), E=22-54 MeV; analyzed σ(θ); deduced optical, l-dependent hybrid potentials coexistence.
doi: 10.1103/PhysRevC.53.3032
1995MI13 Phys.Rev. C51, 3290 (1995) F.Michel, G.Reidemeister, Y.Kondo A Potential Deduced from Low Energy 16O(α, α) Elastic Scattering NUCLEAR REACTIONS 16O(α, α), E=3.5-9.9 MeV; analyzed σ(θ) vs E; deduced model parameters. 20Ne deduced resonances Γ. Real, energy-independent potentials.
doi: 10.1103/PhysRevC.51.3290
1993RE03 Phys.Rev. C47, R1846 (1993) Negative-Parity Inversion Doublet α-Cluster Band in 18O NUCLEAR REACTIONS 14C(α, α), E=28-54 MeV; calculated σ(θ). 14C(α, α), E=3.5-6 MeV; calculated σ(θ) vs E. 18O deduced α-cluster states based band. Global optical model potential.
doi: 10.1103/PhysRevC.47.R1846
1991TA12 Phys.Rev. C44, 477 (1991) N.Takigawa, F.Michel, A.B.Balantekin, G.Reidemeister Dynamic Polarization Potential Induced by the Coulomb Excitation of Deformed Heavy Ions: Geometric scattering approach NUCLEAR REACTIONS 184W(18O, 18O), E=90 MeV; calculated σ(θ). Geometric scattering theory, WKB approximation.
doi: 10.1103/PhysRevC.44.477
1991TA20 Phys.Lett. 262B, 199 (1991) N.Takigawa, F.Michel, A.B.Balantekin, G.Reidemeister A Geometric Approach to Strong Coupling Effects in Heavy-Ion Collisions. Deviation from the Fresnel Diffraction Pattern NUCLEAR REACTIONS 189W(18O, 18O), E=90 MeV; calculated σ(θ); deduced Coriolis coupling role. Geometric approach.
doi: 10.1016/0370-2693(91)91554-9
1990KO18 Phys.Lett. 242B, 340 (1990) Y.Kondo, F.Michel, G.Reidemeister A Unique Deep Potential for the 16O + 16O System NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; calculated σ(θ); deduced model parameters.
doi: 10.1016/0370-2693(90)91772-4
1990RE02 Phys.Rev. C41, 63 (1990) G.Reidemeister, S.Ohkubo, F.Michel Alpha-Cluster Spectroscopy in 40Ca and in the sd-Shell Closure Region NUCLEAR REACTIONS 36Ar(α, α), E=18-41 MeV; analyzed σ(E, θ); deduced optical model parameters. NUCLEAR STRUCTURE 40Ca; calculated α-cluster states, rms radii, B(λ). Discussed other s-d shell nuclei.
doi: 10.1103/PhysRevC.41.63
1989MI06 Phys.Lett. 220B, 479 (1989) F.Michel, Y.Kondo, G.Reidemeister Direct Evidence for a Rapid Energy Dependence of the Nucleus-Nucleus Interaction Near the Barrier Radius at Low Energy NUCLEAR REACTIONS 16O(α, α), E=3.485-4.878 MeV; calculated σ(θ); deduced nucleus-nucleus interaction features.
doi: 10.1016/0370-2693(89)90772-7
1989MI12 Z.Phys. A333, 331 (1989) Evidence for a Parity Dependence of the α + 20Ne Interaction NUCLEAR REACTIONS 20Ne(α, α), E=54.1 MeV; analyzed σ(θ); deduced model parameters. NUCLEAR STRUCTURE 24Mg; calculated rotational bands. α-cluster spectroscopy. 20Ne(α, α) analysis potentials.
1988MI01 Phys.Rev. C37, 292 (1988) F.Michel, G.Reidemeister, S.Ohkubo Potential Description of the Positive- and Negative-Energy Properties of the α + 40Ca System and α-Cluster Structure of 44Ti NUCLEAR STRUCTURE 44Ti; calculated levels, B(E2), α-spectroscopic factors, rms radii, Γ. Local potential model, α+40Ca cluster structure. NUCLEAR REACTIONS 40Ca(α, α), E ≤ 50 MeV; calculated phase shifts. Local potential model, α+40Ca cluster model.
doi: 10.1103/PhysRevC.37.292
1988MI06 Z.Phys. A329, 385 (1988) Connection of Kukulin's Nucleon-Nucleon Deep Potential with Realistic Repulsive Core Interactions NUCLEAR STRUCTURE 2H; calculated binding energy, rms radius, D-state probability, quadrupole moment. Deep nucleon-nucleon potential.
1987MI07 Phys.Rev. C35, 1961 (1987) F.Michel, G.Reidemeister, S.Ohkubo Last Members of the K(π) = 04+ α-Cluster Rotational Band in 20Ne NUCLEAR STRUCTURE 20Ne; calculated rotational bands. α-16O cluster. NUCLEAR REACTIONS, ICPND 16O(α, γ), (α, X), E=15-40 MeV; calculated reaction, fusion σ(E).
doi: 10.1103/PhysRevC.35.1961
1986MI20 Phys.Rev.Lett. 57, 1215 (1986) F.Michel, G.Reidemeister, S.Ohkubo Evidence for Alpha-Particle Clustering in the 44Ti Nucleus NUCLEAR STRUCTURE 44Ti; calculated levels, B(E2), intercluster rms radii; deduced α-clustering effects.
doi: 10.1103/PhysRevLett.57.1215
1986MI21 Phys.Rev. C34, 1248 (1986) F.Michel, G.Reidemeister, S.Ohkubo Molecular Interpretation of the Oscillations of the Fusion Excitation Function for the α + 40Ca System NUCLEAR STRUCTURE 44Ti; calculated bound, quasibound levels; deduced rotational bands. Cluster model. NUCLEAR REACTIONS, ICPND 40Ca(α, α), (α, X), E=10-27 MeV; calculated fusion, reaction σ(E), σ(θ); deduced optical model parameters. 44Ti deduced positive band structure. Optical model analysis.
doi: 10.1103/PhysRevC.34.1248
1985MI11 J.Phys.(London) G11, 835 (1985) Connection between Deep- and Shallow-Type Potential Descriptions of Elastic α Particle Scattering NUCLEAR REACTIONS 16O(α, α), E ≤ 50 MeV; calculated phase shifts; deduced potential parameter optimal values. Microscopic model, antisymmetrization.
doi: 10.1088/0305-4616/11/7/008
1984MI03 Phys.Rev. C29, 1928 (1984) Critique of a Recent Statistical Interpretation of Low Energy 40Ca(α, α) Elastic Scattering NUCLEAR REACTIONS 40Ca(α, α), E=27-33 MeV; analyzed σ(θ); deduced no fluctuation component. Energy-independent, spline real form factor, semi-classical optical model S-matrix decomposition.
doi: 10.1103/PhysRevC.29.1928
1983KL10 Radiochim.Acta 33, 177 (1983) H.Klewe-Nebenius, F.Michel, H.Munzel, G.Pfennig Excitation Functions for the Production of 49V RADIOACTIVITY 49V(EC) [from 51V(p, t), E=14-25 MeV; 51V(d, nt), E=10-25 MeV; 51V(3He, nα), E=0.5-4 MeV; 51V(α, 2nα), E=0.2-2 MeV]; measured I X-ray, Iγ. NUCLEAR REACTIONS, ICPND 51V(p, t), E=14-25 MeV; 51V(d, nt), E=10-25 MeV; 51V(3He, nα), E=0.5-4 MeV; 51V(α, 2nα), E=0.2-2 MeV; measured I X-ray, Iγ; deduced production σ for 49V. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0295. 1983KL11 Radiochim.Acta 33, 181 (1983) H.Klewe-Nebenius, F.Michel, H.Munzel, B.Neumann Monitor Reactions for High Energetic 6Li-Projectiles NUCLEAR REACTIONS, ICPND 27Al(6Li, X)22Na/24Na, E=25-153 MeV; measured σ vs E. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0285. 1983MI22 Phys.Rev. C28, 1904 (1983) F.Michel, J.Albinski, P.Belery, Th.Delbar, Gh.Gregoire, B.Tasiaux, G.Reidemeister Optical Model Description of α + 16O Elastic Scattering and Alpha-Cluster Structure in 20Ne NUCLEAR REACTIONS 16O(α, α), E=39.3-54 MeV; measured σ(θ); deduced optical potential best fit parameters. 20Ne deduced resonance, J, π, α-cluster structure. Global optical model, other data input.
doi: 10.1103/PhysRevC.28.1904
1982AL02 Phys.Rev. C25, 213 (1982) Quantum Calculation of the Barrier and Internal Wave Contributions to Light - and Heavy-Ion Elastic Scattering NUCLEAR REACTIONS 40,44Ca(α, α), E=29 MeV; 90Zr(α, α), E=23.4 MeV; 16O(6Li, 6Li), E=29.8 MeV; 40Ca(16O, 16O), E=54 MeV; 40Ca(12C, 12C), E=47.2, 51 MeV; 28Si(16O, 16O), E=55 MeV; calculated σ(θ). Barrier, internal wave component scattering amplitude decomposition.
doi: 10.1103/PhysRevC.25.213
1981DU07 Nucl.Phys. A355, 141 (1981) F.Duggan, M.Lassaut, F.Michel, N.Vinh Mau Antisymmetrization and Density-Dependent Effects within the Folding Model Approach to α-Nucleus Scattering NUCLEAR REACTIONS 40Ca(α, α), E=104 MeV; calculated σ(θ). Folding model, α-nucleus potential from Hartree-Fock approximation, antisymmetrization, density dependent forces.
doi: 10.1016/0375-9474(81)90135-4
1979MI07 Phys.Lett. 82B, 183 (1979) Investigation of the Deep Interior of the α-Nucleus Interaction Around A = 40 NUCLEAR REACTIONS 40Ca(α, α), E=22-142 MeV; 36,40Ar, 42,44,48Ca(α, α'), E=29 MeV; analyzed σ(θ); deduced optical potentials. Model-independent analysis.
doi: 10.1016/0370-2693(79)90731-7
1978DE25 Phys.Rev. C18, 1237 (1978) T.Delbar, G.Gregoire, G.Paic, R.Ceuleneer, F.Michel, R.Vanderpoorten, A.Budzanowski, H.Dabrowski, L.Freindl, K.Grotowski, S.Micek, R.Planeta, A.Strzalkowski, K.A.Eberhard Elastic and Inelastic Scattering of Alpha Particles from 40,44Ca over A Broad Range of Energies and Angles NUCLEAR REACTIONS 40Ca(α, α), (α, α'), E=40-62 MeV; 44Ca(α, α), E=40-58 MeV; measured σ(θ); deduced optical model parameters. 40Ca deduced β3. Enriched targets.
doi: 10.1103/PhysRevC.18.1237
1977MI07 Phys.Rev. C16, 142 (1977) Optical Model Description of Anomalous Elastic and Inelastic α-40Ca Scattering between 20 and 50 MeV NUCLEAR REACTIONS 40Ca(α, α), (α, α'), E=20-50 MeV; calculated σ(E, θ). Optical model, DWBA analysis.
doi: 10.1103/PhysRevC.16.142
1976MI04 Phys.Lett. 60B, 229 (1976) α-Clustering in the Ground State of 40Ca NUCLEAR REACTIONS 40Ca(α, α), E=18-29 MeV; calculated σ(E, θ).
doi: 10.1016/0370-2693(76)90287-2
1976MI06 Phys.Rev. C13, 1446 (1976) Semimicroscopic Analysis of 44Ca(α, α) from 18.0 to 49.5 MeV NUCLEAR REACTIONS 44Ca(α, α), E=18.0-49.5 MeV; calculated σ(θ); deduced optical model analysis. Folding model analysis.
doi: 10.1103/PhysRevC.13.1446
1975CE01 Phys.Rev. C11, 631 (1975) R.Ceuleneer, F.Michel, M.Bosman, J.Lega, P.Leleux, P.C.Macq, J.P.Meulders, C.Pirart High-Spin States in 20Ne Reached by 16O(α, α)16O Elastic Scattering NUCLEAR REACTIONS 16O(α, α), E=12.8-14.8 MeV; measured σ(E, θ). 20Ne levels deduced J, π.
doi: 10.1103/PhysRevC.11.631
1973CE01 Phys.Lett. 43B, 365 (1973) Regge Poles and Backward Elastic α-Particle Scattering from 16O NUCLEAR REACTIONS 16O(α, α), E=20.4, 28.1, 29.1, 30.0; calculated σ(E, θ). 16O deduced resonances, J, π.
doi: 10.1016/0370-2693(73)90372-9
1970GI02 Nucl.Phys. A145, 337 (1970) J.Gindler, H.Munzel, J.Buschmann, G.Christaller, F.Michel, G.Rohde Fragment Angular Distributions in the Fission of Heavy Nuclei by 103 MeV Helium Ions and 51.5 MeV Deuterons NUCLEAR REACTIONS, Fission 197Au, 209Bi, 233,234,235,238U(α, F), E=103 MeV; 209Bi, 233,234,235,238U(d, F), E=51.5 MeV; measured fission fragment σ(θ), σ(α), F, σ(d), F. Enriched targets.
doi: 10.1016/0375-9474(70)90427-6
1964MI16 Phys.Rev. 133, B329 (1964) Parity Nonconservation in Nuclei
doi: 10.1103/PhysRev.133.B329
1962MA22 Phys.Rev. 127, 545 (1962) Comparison of the Beta Spectra of B12 and N12 NUCLEAR STRUCTURE 12N, 12B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.127.545
1961MA16 Phys.Rev.Letters 7, 167 (1961) Comparison of the Beta Spectra of B12 and N12 NUCLEAR STRUCTURE 12N, 12B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.7.167
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