NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = V.Hnizdo Found 35 matches. 2001CA25 Phys.Rev. C63, 064601 (2001) P.D.Cathers, E.E.Bartosz, M.W.Cooper, N.Curtis, N.Keeley, K.W.Kemper, F.Marechal, E.G.Myers, B.G.Schmidt, K.Rusek, V.Hnizdo First Complete Set of Spin 3/2 Nuclear Scattering Analyzing Powers NUCLEAR REACTIONS 4He(polarized 7Li, 7Li), E(cm)=11.5, 16.5 MeV; measured σ(θ), analyzing powers. Optical model analysis.
doi: 10.1103/PhysRevC.63.064601
1996KE09 Phys.Rev. C54, 1267 (1996) P.L.Kerr, K.W.Kemper, P.V.Green, K.Mohajeri, E.G.Myers, B.G.Schmidt, V.Hnizdo 6Li(pol) + 12C Inelastic Scattering at 30 and 50 MeV NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=30, 50 MeV; measured iT11(θ), T20(θ), T21(θ), T22(θ), σ(θ). 6Li(12C, 12C), E=100 MeV; measured σ(θ); deduced optical model parameters. 6Li, 12C levels deduced deformation length parameters. Coupled channels method.
doi: 10.1103/PhysRevC.54.1267
1995CA26 Nucl.Phys. A591, 349 (1995) J.Carter, Z.Z.Vilakazi, R.W.Fearick, V.Hnizdo, E.Muskat, K.W.Kemper, D.E.Trcka, S.P.Van Verst Elastic and Inelastic Scattering in the 6Li, 9Be + 12C Systems: Excitation of unbound excited states and cluster transfers NUCLEAR REACTIONS 12C(9Be, 9Be), (9Be, 9Be'), 9Be(12C, 12C), (12C, 12C'), E(cm)=3-16 MeV; 12C(6Li, 6Li), (6Li, 6Li'), E(cm)=2-16 MeV; measured σ(θ) vs E. 12C, 9Be, 6Li levels deduced deformation lengths. Finite-range DWBA, Woods-Saxon potential, double-folded real potential, coupled-channels calculations, compound-nucleus calculations, 3He-cluster transfers.
doi: 10.1016/0375-9474(95)00199-B
1995MU01 Nucl.Phys. A581, 42 (1995) E.Muskat, J.Carter, R.W.Fearick, V.Hnizdo Inelastic Scattering in the 6Li + 9Be System Leading to Unbound Excited States of Either Nucleus NUCLEAR REACTIONS 9Be(6Li, 6Li), (6Li, 6Li'), E(cm)=7, 10, 12 MeV; measured σ(θ) vs E. 9Be levels deduced deformation lengths. Coupled-channels, double-folded real potential. Compound-nucleus calculations, triton-cluster transfers, finite-range DWBA.
doi: 10.1016/0375-9474(94)00323-F
1994EN06 Phys.Rev.Lett. 73, 3508 (1994) Microscopic T-Violating Optical Potential: Implications for neutron-transmission experiments NUCLEAR REACTIONS 165Ho(polarized n, X), E not given; calculated T-violating ρ-nucleon coupling limits, transmission experiments. Microscopic T-violating optical potential.
doi: 10.1103/PhysRevLett.73.3508
1994HN01 Phys.Rev. C49, R612 (1994) Optical-Model Description of Time-Reversal Violation in Neutron-Nucleus Scattering NUCLEAR REACTIONS 165Ho(n, n), E ≤ 20 MeV; calculated σ(E); 165Ho(polarized n, n), E ≤ 20 MeV; calculated T-odd spin-correlation coefficient vs E. Optical model.
doi: 10.1103/PhysRevC.49.R612
1994HN02 Phys.Rev. C50, 1251 (1994) Differences between the Deformed-Potential and Folding-Model Descriptions of Inelastic Nuclear Scattering
doi: 10.1103/PhysRevC.50.1251
1994HN03 Phys.Rev. C50, 2639 (1994) Observables for Polarized Neutrons Transmitted Through Polarized Targets
doi: 10.1103/PhysRevC.50.2639
1994RE15 Phys.Rev. C50, 2917 (1994) E.L.Reber, K.W.Kemper, P.V.Green, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt, V.Hnizdo Analyzing Powers for Elastic and Inelastic Scattering of Polarized 6Li from 12C at 30 MeV NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=30 MeV; measured σ(θ), vector, tensor analyzing power vs θ. 6Li, 12C levels deduced deformation lengths. Coupled-channels analysis.
doi: 10.1103/PhysRevC.50.2917
1993RE08 Phys.Rev. C48, 285 (1993) E.L.Reber, K.W.Kemper, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt, V.Hnizdo Analyzing Powers for Elastic and Inelastic Scattering of Polarized 6Li from 9Be at 32 MeV NUCLEAR REACTIONS 9Be(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=32 MeV; measured vector, tensor analyzing power vs θ; deduced optical potential constraints, parameters. Coupled-channels calculations.
doi: 10.1103/PhysRevC.48.285
1989VA04 Phys.Rev. C39, 853 (1989) S.P.Van Verst, D.P.Sanderson, D.E.Trcka, K.W.Kemper, V.Hnizdo, B.G.Schmidt, K.R.Chapman Vector Polarized 6Li Scattering from 12C and 16O NUCLEAR REACTIONS 16O(polarized 6Li, 6Li), E=25.7 MeV; 12C(polarized 6Li, 6Li), E=30 MeV; measured σ(θ), analyzing power vs θ; deduced reaction mechanism, model parameters.
doi: 10.1103/PhysRevC.39.853
1988CO16 Phys.Rev. C38, 1619 (1988) P.D.Cottle, V.Hnizdo, R.J.Philpott, K.A.Stuckey, K.W.Kemper, J.A.Carr Negative Parity States of Even-A Pt Isotopes from Proton Inelastic Scattering NUCLEAR REACTIONS 194,196,198Pt(p, p'), E=35 MeV; analyzed σ(θ); deduced 3- state systematics in Os, Pt, Hg region. 194,196,198Pt level deduced β3, B(E3).
doi: 10.1103/PhysRevC.38.1619
1988HN01 Phys.Rev. C38, 1242 (1988) Spin-Spin Effects through Nuclear Reorientation in Elastic Scattering of Deformed Heavy Ions NUCLEAR REACTIONS 11B(7Li, X), E=30-38 MeV; calculated total spin-spin reaction σ(E). Quadrupole-quadrupole moment interaction, heavy-ions.
doi: 10.1103/PhysRevC.38.1242
1987HN01 J.Phys.(London) G13, 27 (1987) On the Optical-Potential Deformation in Heavy-Ion Inelastic Scattering NUCLEAR REACTIONS 24Mg(16O, 16O'), E=29 MeV; 28Si(16O, 16O'), E=32 MeV; calculated σ(θ); deduced model parameters. DWBA, coupled-channels calculations.
doi: 10.1088/0305-4616/13/1/006
1987HN02 Phys.Rev.Lett. 59, 1892 (1987) Spin-Spin Dependence of Total Cross Sections as an Effect of Static Nuclear Deformation NUCLEAR REACTIONS 27Al(polarized n, X), E=2-20 MeV; calculated spin-spin total σ(E). Coupled-channels calculations, polarized target.
doi: 10.1103/PhysRevLett.59.1892
1986CA24 Nucl.Phys. A460, 341 (1986) B.O.Carragher, J.Carter, R.G.Clarkson, V.Hnizdo, J.P.F.Sellschop A Study of the α-Transfer Reaction in the 16O + 16O System at Near-Barrier Energies NUCLEAR REACTIONS 16O(16O, 16O), (16O, 12C), E=11-18 MeV; measured σ(θ), σ(E). 20Ne levels deduced spectroscopic factors. DWBA analysis, double folded real, Woods-Saxon optical potentials.
doi: 10.1016/0375-9474(86)90130-2
1986HN01 Phys.Lett. 167B, 26 (1986) On the Determination of the Nuclear Forward Amplitude and Total Reaction Cross Section from Heavy-Ion Elastic Scattering NUCLEAR REACTIONS 12C(12C, 12C), E(cm)=20 MeV; 28Si(16O, 16O), E(cm)=35 MeV; calculated σ(θ), reaction σ; deduced nuclear forward amplitude. Generalized optical theorem.
doi: 10.1016/0370-2693(86)90538-1
1983CO05 Phys.Rev. C27, 1536 (1983) J.Cook, M.F.Vineyard, K.W.Kemper, V.Hnizdo Quadrupole Effects in 7Li Scattering at 88 MeV NUCLEAR REACTIONS 24,26Mg, 40,48Ca(7Li, 7Li), E=88 MeV; calculated σ(θ); deduced quadrupole term role in optical potentials. Double-folding model analysis.
doi: 10.1103/PhysRevC.27.1536
1981HN01 Phys.Rev. C23, 236 (1981) V.Hnizdo, C.W.Glover, K.W.Kemper Inelastic Scattering of 11B from 40Ca NUCLEAR REACTIONS 40Ca(11B, 11B), (11B, 11B'), E=51.5 MeV; measured σ(θ). 11B, 40Ca levels deduced deformation lengths. DWBA, coupled-channels, double folding model analyses.
doi: 10.1103/PhysRevC.23.236
1981HN02 Phys.Rev.Lett. 46, 590 (1981) V.Hnizdo, K.W.Kemper, J.Szymakowski Quadrupole Effects in 7Li and 9Be Scattering and the Folding Model NUCLEAR REACTIONS 54Fe(7Li, 7Li), (7Li, 7Li'), E=48 MeV; 40Ca(7Li, 7Li), E=34 MeV; 40Ca(9Be, 9Be), E=40 MeV; analyzed σ(θ); deduced optical model parameters, projectile quadrupole moment effects. 9Be, 7Li levels deduced deformation lengths. Coupled-channels method, unrenormalized real double folded potential.
doi: 10.1103/PhysRevLett.46.590
1981HN04 Phys.Rev. C24, 1495 (1981) V.Hnizdo, J.Szymakowski, K.W.Kemper, J.D.Fox Folding-Model Description of Elastic and Inelastic Scattering of 9Be by 40,44Ca and 39K at 40 MeV NUCLEAR REACTIONS 39K, 40,44Ca(9Be, 9Be), (9Be, 9Be'), E=40 MeV; measured σ(θ). 40,44Ca, 39K deduced deformation length. DWBA analysis, double folding model.
doi: 10.1103/PhysRevC.24.1495
1979HN01 Nucl.Phys. A315, 233 (1979) V.Hnizdo, C.Toepffer, A.Richter, O.Titze Small Deviations from Rutherford Scattering NUCLEAR REACTIONS 208Pb(α, α), E=16 MeV; 208Pb(16O, 16O), E=69 MeV; calculated σ(θ), optical potentials including deviations from point charge; deduced Coulomb potential; deduced nuclear contributions cancel vacuum polarization effects.
doi: 10.1016/0375-9474(79)90645-6
1978CA07 Nucl.Phys. A297, 520 (1978) J.Carter, R.G.Clarkson, V.Hnizdo, J.P.F.Sellschop Inelastic Scattering of Heavy Ions from Deformed Light Nuclei at Near-Barrier Energies NUCLEAR REACTIONS 24Mg(18O, 18O), E=29, 35 MeV; 28Si(12C, 12C), E=24, 29 MeV; 28Si(16O, 16O), E=32 MeV; 28Si(18O, 18O), E=40 MeV; measured σ(θ); deduced optical model potentials. DWBA, closed formalism, coupled channels analysis. Enriched targets.
doi: 10.1016/0375-9474(78)90157-4
1978SE16 S.Afr.J.Phys. 1, 202 (1978) J.P.F.Sellschop, J.Carter, R.G.Clarkson, V.Hnizdo, A.Howes Anomalous Large-Angle Scattering and Quasi-Molecular States in the α 40Ca System NUCLEAR REACTIONS 40Ca(α, α), E=6-18 MeV; measured σ(θ, E); deduced quasimolecular resonances. Resonating group theory.
1978VO06 Nucl.Phys. A307, 309 (1978) C.Von Charzewski, V.Hnizdo, C.Toepffer Symmetry and Shell Effects in Heavy-Ion Scattering NUCLEAR REACTIONS 16O(16O, 16O), 18O(18O, 18O), 12C(20Ne, 20Ne), E(cm) ≈ 22 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(78)90620-6
1978VO13 S.Afr.J.Phys. 1, 222 (1978) C.von Charzewski, V.Hnizdo, C.Toepffer Effects of Symmetry and Shell Structure on Absorption in Heavy-Ion Scattering NUCLEAR REACTIONS 16O(16O, 16O), 18O(18O, 18O), 20Ne(12C, 12C), E(cm)=16-28 MeV; calculated σ(θ, E). Precompound state density dependent absorptive potentials.
1977OS02 Phys.Lett. 68B, 319 (1977) F.Osterfeld, V.Hnizdo, C.Toepffer Is the Difference between 12C-20Ne and 16O-16O Scattering Due to Entrance Channel Effects (Question) NUCLEAR REACTIONS 20Ne(12C, 12C); calculated σ(θ).
doi: 10.1016/0370-2693(77)90484-1
1976CA30 Nucl.Phys. A273, 523 (1976) J.Carter, R.G.Clarkson, V.Hnizdo, R.J.Keddy, D.W.Mingay, F.Osterfeld, J.P.F.Sellschop Elastic and Inelastic Scattering of 16O and 12C by 24Mg Near the Coulomb Barrier NUCLEAR REACTIONS 24Mg(16O, 16O), E=28, 29, 30, 33 MeV; 24Mg(12C, 12C), E=21, 24 MeV; measured σ(θ) for ground state, first 2+ in 24Mg; deduced optical model potentials. DWBA, ICC analysis. Enriched target.
doi: 10.1016/0375-9474(76)90608-4
1972GR02 Nucl.Phys. A179, 1 (1972) P.D.Greaves, V.Hnizdo, J.Lowe, O.Karban Elastic and Inelastic Scattering of 30.4 MeV Polarised Protons by 12,13C, 16O and 54Fe NUCLEAR REACTIONS 12C, 13C, 16O, 54Fe(polarized p, p), (polarized p, p'); measured σ(θ), P(θ), analyzing power(θ); deduced effective interactions.Enriched targets.
doi: 10.1016/0375-9474(72)90101-7
1971HN02 Phys.Rev. C3, 1560 (1971) V.Hnizdo, O.Karban, J.Lowe, G.W.Greenlees, W.Makofske Elastic Scattering of 30.3-MeV Polarized Protons from 40Ca, 56Fe, and 59Co NUCLEAR REACTIONS 40Ca, 56Fe, 59Co(polarized p, p), E=30.3 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1103/PhysRevC.3.1560
1971HN03 Phys.Lett. 35B, 35 (1971) Collective-Model Analysis of Inelastic Proton Scattering Using Potentials Derived from Nuclear Matter Distributions NUCLEAR REACTIONS 56Fe, 58Ni, 120Sn, 208Pb(polarized p, p), E=30.3 MeV; measured nothing; analyzed σ(θ), asymmetry(θ). Collective model analysis.
doi: 10.1016/0370-2693(71)90433-3
1970GR24 Phys.Rev. C2, 1063 (1970) G.W.Greenlees, V.Hnizdo, O.Karban, J.Lowe, W.Makofske Elastic Scattering of 30.3-MeV Polarized Protons from 58Ni, 120Sn, and 208Pb NUCLEAR REACTIONS 58Ni, 120Sn, 208Pb(polarized p, p), E=30.3 MeV; measured σ(θ), P(θ).
doi: 10.1103/PhysRevC.2.1063
1970KA10 Nucl.Phys. A147, 461 (1970) O.Karban, P.D.Greaves, V.Hnizdo, J.Lowe, G.W.Greenlees Inelastic Scattering of Polarized Protons at 30.3 MeV by 54,56Fe, 58Ni, 120Sn and 208Pb NUCLEAR REACTIONS 54,56Fe, 58Ni, 120Sn, 208Pb(polarized p, p'), E=30.3 MeV; measured σ(θ), asymmetry (θ). 54,56Fe, 58Ni, 120Sn, 208Pb deduced nuclear deformations β(L). Enriched targets.
doi: 10.1016/0375-9474(70)90592-0
1969KA14 Nucl.Phys. A132, 548 (1969) O.Karban, P.D.Greaves, V.Hnizdo, J.Lowe, N.Berovic, H.Wojciechowski, G.W.Greenlees The Elastic Scattering of Protons by 16O in the Energy Range 16-30 MeV NUCLEAR REACTIONS 16O(p, p), E=16-30.5 MeV; measured σ(E, θ). 16O(polarized p, p), E=19.8-22.1, 30.3 MeV; measured P(E, θ). 17F resonances deduced J, π.
doi: 10.1016/0375-9474(69)90717-9
1969KA15 Nucl.Phys. A133, 255 (1969); Erratum Nucl.Phys. A141, 675 (1970) O.Karban, J.Lowe, P.D.Greaves, V.Hnizdo Polarisation in 11B(p, p) and 11B(p, p') at 30.3 MeV NUCLEAR REACTIONS 11B(polarized p, p), 11B(polarized p, p'), E= 30.3 MeV; measured σ(Ep, θ), asymmetry (θ). Enriched target.
doi: 10.1016/0375-9474(69)90629-0
Back to query form |