NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = E.Wesolowski Found 13 matches. 2001MO05 Phys.Rev. C63, 034302 (2001) T.Morek, J.Srebrny, Ch.Droste, M.Kowalczyk, T.Rzaca-Urban, K.Starosta, W.Urban, R.Kaczarowski, E.Ruchowska, M.Kisielinski, A.Kordyasz, J.Kownacki, M.Palacz, E.Wesolowski, W.Gast, R.M.Lieder, P.Bednarczyk, W.Meczynski, J.Styczen Investigation of the Kπ = 8- Isomer in 132Ce NUCLEAR REACTIONS 120Sn(16O, 4n), E=80 MeV; measured delayed Eγ, Iγ(t), γγ-coin. 132Ce deduced levels, J, π, T1/2 and hindrance factor for high-K isomer. Systematics of isomers in mass region discussed.
doi: 10.1103/PhysRevC.63.034302
1999DR12 Nucl.Instrum.Methods Phys.Res. A430, 260 (1999) Ch.Droste, K.Starosta, A.Wierzchucka, T.Morek, S.G.Rohozinski, J.Srebrny, M.Bergstrom, B.Herskind, E.Wesolowski PPCO: Polarization-Polarization Correlation from Oriented Nuclei NUCLEAR REACTIONS 138Ba(30Si, 4n), E not given; analyzed γ-ray polarization, correlations from oriented nuclei. Eurogam II segmented detectors.
doi: 10.1016/S0168-9002(99)00224-7
1991WE07 J.Phys.(London) G17, 955 (1991) E.Wesolowski, A.Saganek, E.Gierlik, V.Meyer, M.Sieminski, A.Turowiecki, Z.Wilhelmi Neutron Distribution Differences of Nickel Isotopes NUCLEAR REACTIONS 60,62,64Ni(d, p), E=2.7, 3, 3.3 MeV; measured σ(θ). 60,62,64Ni deduced single particle wavefunctions, density of valence neutrons, neutron isotope density differences. Enriched Ni targets. DWBA analysis.
doi: 10.1088/0954-3899/17/6/016
1987TU01 Nucl.Phys. A468, 29 (1987) A.Turowiecki, A.Saganek, M.Sieminski, E.Wesolowski, Z.Wilhelmi The 11B(α, p)14C Reaction below 1.7 MeV bombarding Energy NUCLEAR REACTIONS, ICPND 11B(α, p), E=0.9-1.7 MeV; measured residual production σ(E). 15N deduced resonances, partial widths.
doi: 10.1016/0375-9474(87)90316-2
1986GO02 Phys.Rev. C33, 793 (1986) I.M.Govil, H.W.Fulbright, D.Cline, E.Wesolowski, B.Kotlinski, A.Backlin, K.Gridnev Multipole Collectivity in 168Er from Inelastic Scattering NUCLEAR REACTIONS 168Er(α, α), (α, α'), E=36 MeV; 168Er(d, d), (d, d'), E=16 MeV; measured σ(θ), σ(Eα'); deduced optical model parameters. 168Er deduced octupole states, β4, β6 shape components, B(λ). Coupled-channels calculation, collective model form factors.
doi: 10.1103/PhysRevC.33.793
1986WE13 Acta Phys.Pol. B17, 1101 (1986) E.Wesolowski, A.Saganek, M.Sieminski The Sharp Radius, Effective Interaction Range and the Volume Integral of the Shell Model Potential NUCLEAR STRUCTURE A=36-65; calculated shell model potential, volume integral, radius parameter; deduced mass dependence. Optical model input.
1985SA33 J.Phys.(London) G11, 1221 (1985) A.Saganek, V.Meyer, S.A.Said, M.Sieminski, A.Turowiecki, E.Wesolowski, Z.Wilhelmi Neutron Orbit Radii in 99Mo from the (d, p) Sub-Coulomb Reaction NUCLEAR REACTIONS 98Mo(d, p), E=4.5 MeV; measured σ(θ), σ(Ep); deduced opticial model parameters. 99Mo levels deduced reduced normalization, neutron orbit rms radii.
doi: 10.1088/0305-4616/11/11/009
1985WE09 J.Phys.(London) G11, 909 (1985) The RMS Radii of the Charge Distribution in Nuclei NUCLEAR STRUCTURE Z ≥ 5; N ≥ 5; calculated charge distribution rms radii. Semi-empirical formula.
doi: 10.1088/0305-4616/11/8/008
1984SA05 J.Phys.(London) G10, 549 (1984) A.Saganek, V.Meyer, S.Mirowski, M.Oteski, M.Sieminski, E.Wesolowski, Z.Wilhelmi Neutron Orbit Radii in 89Sr from the (d, p) Sub-Coulomb Reaction NUCLEAR REACTIONS 88Sr(d, p), E=3.4, 3.8, 4 MeV; measured σ(θ), σ(Ep), absolute σ; deduced optical potential parameters. 89Sr levels deduced spectroscopic, normalization factors, neutron orbit rms radii. DWBA analysis.
doi: 10.1088/0305-4616/10/4/015
1984WE01 J.Phys.(London) G10, 181 (1984) The Effective Two-Body Interaction Range Derived from the Proton Optical-Model Parameters NUCLEAR STRUCTURE A=20-210; analyzed proton optical potentials ; deduced two-body interaction range mass, potential depth dependences, energy parameter mass dependence.
doi: 10.1088/0305-4616/10/2/009
1984WE04 J.Phys.(London) G10, 321 (1984) The RMS Radii of Nuclear Proton Distributions NUCLEAR STRUCTURE A=12-70; Z=6-30; calculated proton, charge distribution rms radii. 41,43,45,47Ca, 47,49Ti, 74,76Ge, 76,78,80,82Se, 78,80,82,84,86Kr, 77,79,81,83,85,87Rb, 68Zn; calculated rms charge radii. Semi-empirical model.
doi: 10.1088/0305-4616/10/3/008
1984WE13 Acta Phys.Pol. B15, 559 (1984) The Quadrupole Deformation Parameters of Charge Distributions in Nuclei NUCLEAR STRUCTURE A=20-240; calculated β2, B(E2); deduced mass dependence. Semi-empirical model.
1976WE29 Acta Phys.Pol. B7, 633 (1976) Shell and Excitation Energy Effects in the Potential Radii Deduced from (d, p) Reactions on s-d Shell Nuclei at Low Deuteron Energy NUCLEAR REACTIONS 23Na, 24,26Mg, 27Al, 28Si, 31P, 32,34S, 35Cl(d, p), E=2.4, 2.5, 2.6 MeV; measured σ(Ep, θ). 25Mg, 27Mg, 29Si levels deduced β.
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