NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = W.Savin Found 16 matches. 1978BA20 Phys.Rev. C17, 1559 (1978) F.T.Baker, A.Scott, R.M.Ronningen, T.H.Kruse, R.Suchannek, W.Savin 192Pt(α, α') Reaction at E = 24 MeV NUCLEAR REACTIONS 192Pt(α, α'), E=24 MeV; measured σ(Eα', θ). 192Pt levels deduced β, relative signs of matrix elements. Coupled channels analysis. Enriched target.
doi: 10.1103/PhysRevC.17.1559
1978RO02 Phys.Rev.Lett. 40, 364 (1978) R.M.Ronningen, F.T.Baker, A.Scott, T.H.Kruse, R.Suchannek, W.Savin, J.H.Hamilton Evidence for a Nonrotational Interpretation of [0+ m(E4) 4+] in 180Hf NUCLEAR REACTIONS 180Hf(α, α'), E=21, 24 MeV; measured σ(Eα', θ). 180Hf levels deduced β2, β4.
doi: 10.1103/PhysRevLett.40.364
1977BA58 Phys.Lett. 70B, 167 (1977) F.T.Baker, A.Scott, R.M.Ronningen, T.H.Kruse, R.Suchannek, W.Savin, J.H.Hamilton Sensitivity of (α, α') Cross Sections to Excited-State Quadrupole Moments NUCLEAR REACTIONS 180Hf(α, α'), E=21, 24 MeV; measured σ(Eα', θ). 180Hf level deduced β.
doi: 10.1016/0370-2693(77)90512-3
1976BA23 Phys.Rev.Lett. 37, 193 (1976) F.T.Baker, A.Scott, T.H.Kruse, W.Hartwig, E.Ventura, W.Savin Experimental Determination of the Signs of E2 Interference Terms for 192Os and 194Pt NUCLEAR REACTIONS 192Os, 194Pt(α, α'), E=12-24 MeV; analyzed data. 192Os, 194Pt deduced sign of interference term.
doi: 10.1103/PhysRevLett.37.193
1976BA35 Nucl.Phys. A266, 337 (1976) F.T.Baker, A.Scott, T.H.Kruse, W.Hartwig, E.Ventura, W.Savin Nuclear Shapes of the Transitional Nuclei 194,196,198Pt NUCLEAR REACTIONS 194,196,198Pt(α, α'), E=14-24 MeV, θlab=127.5°; measured σ(E, e'). 194,196,198Pt deduced β2, β4 charge, mass deformations. 194Pt deduced sign of interference term.
doi: 10.1016/0375-9474(76)90362-6
1975BA09 Phys.Rev. C11, 1051 (1975) F.T.Baker, T.H.Kruse, W.Hartwig, M.E.Williams, W.Savin Coulomb-Nuclear Interference for the 58Ni(14N, 14N') Reaction NUCLEAR REACTIONS 58Ni(14N, 14N), E=30-48 MeV; measured σ(E), first 2+ state at θ(lab)=59°. 58Ni(14N, 14N), E=41 MeV; measured σ(θ). Enriched target.
doi: 10.1103/PhysRevC.11.1051
1974BA78 Nucl.Phys. A235, 428 (1974) F.T.Baker, T.H.Kruse, M.E.Williams, W.Savin Coulomb-Nuclear Interference for Inelastic Deuteron Scattering NUCLEAR REACTIONS 54,56Fe, 60Ni, 114Cd, 152Sm, 192Os(d, d'), E=3-16 MeV; measured σ(E, Ed'). 54,56Fe, 60Ni, 114Cd, 152Sm, 192Os levels deduced deformation lengths βL R. Enriched targets.
doi: 10.1016/0375-9474(74)90203-6
1974MA18 Nucl.Phys. A223, 221 (1974) J.L.Matthews, T.Kruse, M.E.Williams, R.O.Owens, W.Savin Radiative Capture of Protons by Deuterons at E = 16 MeV NUCLEAR REACTIONS 2H(p, γ), E=16 MeV; measured σ(θ).
doi: 10.1016/0375-9474(74)90411-4
1973BA39 Phys.Rev.Lett. 31, 721 (1973) F.T.Baker, T.H.Kruse, M.E.Williams, W.Savin Observation of Nuclear Structure Dependence of the Phase of the (d, d') Form Factor NUCLEAR REACTIONS 54,56Fe, 60Ni, 114Cd, 138Ba, 144,150,152Sm, 192Os(d, d'); measured σ(E). 138Ba, 144,150Sm deduced levels, J, π, deformation parameters.
doi: 10.1103/PhysRevLett.31.721
1973WI16 Nucl.Phys. A213, 317 (1973) M.E.Williams, T.H.Kruse, P.Goode, F.T.Baker, J.L.Matthews, W.Savin Neutron Correlations in the 41K Ground State and T = 1 2p-2h States in 40K NUCLEAR REACTIONS 41K(p, d), (d, t), E=15 MeV; measured σ(θ). 40K levels deduced L, S.
doi: 10.1016/0375-9474(73)90153-X
1972BA61 Phys.Lett. 40B, 355 (1972) F.T.Baker, T.H.Kruse, M.E.Williams, J.L.Matthews, W.Savin The Phase and Shape of the Form Factor for Inelastic 3He Scattering NUCLEAR REACTIONS 114Cd(3He, 3He), (3He, 3He'), E=10-17 MeV; measured σ(E;θ); deduced nuclear/Coulomb excitation interference, form factor.
doi: 10.1016/0370-2693(72)90818-0
1972FE06 Nucl.Phys. A187, 123 (1972) J.A.Fenton, T.H.Kruse, N.Williams, M.E.Williams, R.N.Boyd, W.Savin Two-Hole Strengths in 38K from the 39K(3He, α)38K Reaction NUCLEAR REACTIONS 39K(3He, α)38K, E=21.09 MeV; measured σ(θ(α)), Q. 38K deduced levels, J, π, L(n), T, S. Natural target.
doi: 10.1016/0375-9474(72)90078-4
1971BO10 Nucl.Phys. A162, 497 (1971) R.N.Boyd, J.Fenton, M.Williams, T.Kruse, W.Savin Nuclear Matter Radii in the Tin Isotopes NUCLEAR REACTIONS 116,118,120,124Sn(p, p), E=16.00 MeV; measured P(θ); deduced optical model parameters. 116,118,120,124Sn deduced nuclear matter radii.
doi: 10.1016/0375-9474(71)90250-8
1971KR10 Nucl.Phys. A169, 177 (1971) T.Kruse, W.Makofske, H.Ogata, W.Savin, M.Slagowitz, M.Williams, P.Stoler Elastic and Inelastic Proton Scattering from Heavy Collective Nuclei NUCLEAR REACTIONS 148,150,152,154Sm, 165Ho, 172,174,176Yb, 182,184,186W, 188,190,192Os, 194,198Pt(p, p), (p, p'), Ep=16 MeV; measured σ(θ); deduced optical model parameters. 148,150,152,154Sm, 165Ho, 172,174,174,176Yb, 182,184,186W, 188,190,192Os, 194,198Pt deduced β2 . Enriched target.
doi: 10.1016/0375-9474(71)90570-7
1968MA34 Phys.Rev. 174, 1429 (1968) W.Makofske, W.Savin, H.Ogata, T.H.Kruse Elastic and Inelastic Proton Scattering from Even Isotopes of Cd, Sn, and Te NUCLEAR REACTIONS 110,112,114,116Cd, 112,116,118,120,122,124Sn, 126,128,130Te(p, p'), E=16 MeV; measured σ(θ).
doi: 10.1103/PhysRev.174.1429
1967MA23 Phys.Letters 25B, 322 (1967) W.Makofske, M.Slagowitz, W.Savin, H.Ogata, T.H.Kruse, T.Tamura Scattering of 16-MeV Protons from Even Tin Isotopes NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(p, p'), E=16 MeV; measured σ(θ). Coupled-channel analysis.
doi: 10.1016/0370-2693(67)90082-2
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