NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = F.T.Baker Found 72 matches. 2000BA18 Phys.Rev. C61, 037302 (2000) F.T.Baker, L.Bimbot, G.Edwards, C.Glashausser, A.Green, K.W.Jones, D.Mihailidis, D.Read, A.Sethi, B.H.Storm, Jr., R.de Swiniarski Spin Excitations in the 40Ca(p(pol), p(pol)') Reaction Revisited NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319 MeV; measured σ(E, θ), spin flip probabilities. Comparison with RPA, DWIA calculations.
doi: 10.1103/PhysRevC.61.037302
1999DJ01 Phys.Rev. C59, 118 (1999) C.Djalali, M.Morlet, N.Marty, J.Van de Wiele, A.Willis, F.T.Baker, L.Bimbot, C.Glashausser, J.Guillot, H.Langevin-Joliot, L.Rosier, E.Tomasi-Gustafsson Isoscalar Spin Excitation in 90Zr and 208Pb NUCLEAR REACTIONS 90Zr, 208Pb(polarized d, d), (polarized d, d'), E=400 MeV; measured σ(E, θ), Ay(E, θ), Ayy(E, θ); deduced optical potential parameters. 90Zr, 208Pb deduced spin excitation distributions, spin-flip probability, S=0, S=1 cross sections. DWBA-RPA analysis.
doi: 10.1103/PhysRevC.59.118
1997BB17 Phys.Rep. 289, 235 (1997) F.T.Baker, L.Bimbot, C.Djalali, C.Glashausser, H.Lenske, W.G.Love, M.Morlet, E.Tomasi-Gustafsson, J.Van de Wiele, J.Wambach, A.Willis The Nuclear Spin Response to Intermediate Energy Protons and Deuterons at Low Momentum Transfer NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319, 800 MeV; 12C(polarized p, p'), E=318 MeV; 12C, 40Ca(polarized d, d'), E=400 MeV; analyzed σ(E, θ), spin-tranfer observables; deduced collective effects, nuclear spin response related features.
doi: 10.1016/S0370-1573(97)00008-2
1995JO06 Phys.Rev. C51, 1726 (1995) B.N.Johnson, M.Morlet, C.Djalali, F.T.Baker, L.Bimbot, C.Glashausser, J.Guillot, H.Langevin-Joliot, N.Marty, L.Rosier, E.Tomasi-Gustafsson, J.Van de Wiele, A.Willis Isoscalar Spin Strength in 12C Measured in 400 MeV Deuteron Inelastic Scattering NUCLEAR REACTIONS 12C(polarized d, d'), E=400 MeV; measured σ(E, θ), vector, tensor analyzing power, polarization transfer coefficients vs θ, E. 12C levels deduced spin-flip probability ΔS=0 and ΔS=1 strength, relative spin response (R(S))0. DWIA analysis.
doi: 10.1103/PhysRevC.51.1726
1994GI09 Nucl.Phys. A577, 227c (1994) R.Gilman, E.Brash, G.Edwards, C.Glashausser, M.K.Jones, F.T.Baker, S.Bastea, D.P.Beatty, L.Bimbot, J.Brusoe, J.Chiba, D.Cooper, G.Kumbartzki, C.Mauger, T.Nagae, B.Park, D.Prout, R.D.Ransome, M.Rawool-Sullivan, P.Rutt, B.Storm, E.Sugarbaker, T.Taddeucci, J.Zumbro Coherent Pion Production in 12C(p, nπ) at 800 MeV NUCLEAR REACTIONS 12C(p, nπ+), E=800 MeV; measured neutron, pion spectra.
doi: 10.1016/0375-9474(94)90860-5
1994JO07 Phys.Rev. C50, 1982 (1994) K.W.Jones, C.Glashausser, R.de Swiniarski, F.T.Baker, T.A.Carey, J.R.Comfort, W.Cornelius, J.L.Escudie, M.Gazzaly, A.Green, M.Haji-Saeid, N.Hintz, G.Igo, J.B.McClelland, J.M.Moss, S.Nanda, C.A.Whitten Energy Dependence of the 12C(p, p')12C(*) Reaction from 200 to 800 MeV NUCLEAR REACTIONS 12C(polarized p, p'), E=200-800 MeV; measured σ(E, θ), analyzing power vs (E, θ). DWIA analysis.
doi: 10.1103/PhysRevC.50.1982
1994MO21 Nucl.Phys. A577, 155C (1994) M.Morlet, C.Djalali, E.Tomasi-Gustafsson, A.Willis, J.Van de Wiele, N.Marty, C.Glashausser, B.N.Johnson, F.T.Baker, L.Bimbot, J.Guillot, F.Jourdan, H.Langevin-Joliot, L.Rosier Recent Results on the Isoscalar Spin Response in 40Ca and 12C NUCLEAR REACTIONS 12C(polarized d, d'), E=400 MeV; measured σ(θ), analyzing power, spin-transfer signatures vs θ; 40Ca(polarized d, d'), E not given; analyzed σ(θ), other data. 12C, 40Ca deduced ΔS=1, ΔT=0 strength distribution.
doi: 10.1016/0375-9474(94)90849-4
1993BA37 Phys.Rev. C48, 1106 (1993) F.T.Baker, D.Beatty, L.Bimbot, V.Cupps, C.Djalali, R.W.Fergerson, C.Glashausser, G.Graw, A.Green, K.Jones, M.Morlet, S.K.Nanda, A.Sethi, B.H.Storm, W.Unkelbach, A.Willis Separation of ΔS = 0 and ΔS = 1 in the Response of 12C to 318 MeV Protons NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=318 MeV; measured σ(θ, Ep), spin-flip probability; deduced model parameters. 12C deduced ΔS=0, ΔS=1 multipole transition strength distributions. RPA, DWIA analysis.
doi: 10.1103/PhysRevC.48.1106
1993DE31 Nuovo Cim. 106A, 1119 (1993) R.De Swiniarski, F.T.Baker, A.Scott, C.Glashausser, K.W.Jones Elastic and Inelastic Scattering of 0.8 GeV Polarized Protons from 18O NUCLEAR REACTIONS 18O(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 18O level deduced L. Dirac equation based coupled-channels calculation.
doi: 10.1007/BF02773499
1993GR02 Phys.Rev.Lett. 70, 734 (1993) A.Green, W.Unkelbach, F.T.Baker, D.Beatty, L.Bimbot, X.Y.Chen, V.R.Cupps, C.Djalali, G.Edwards, R.W.Fergerson, C.Glashausser, K.W.Jones, M.K.Jones, G.Kumbartzki, A.Sethi, B.Storm, J.Wambach Spin-Longitudinal and Spin-Transverse Response of 40Ca to 500 MeV Protons at Low Momentum Transfer NUCLEAR REACTIONS 40Ca(polarized p, p'), E=497, 581 MeV; measured spin-transfer observables; deduced longitudinal, transverse spin-flip probabilities. DWIA analysis, finite nucleus RPA.
doi: 10.1103/PhysRevLett.70.734
1993KE03 Phys.Rev. C47, 2146 (1993) J.J.Kelly, B.S.Flanders, F.W.Hersman, J.H.Heisenberg, J.Calarco, J.P.Connelly, T.E.Milliman, A.Scott, F.T.Baker, V.Penumetcha, W.P.Jones, G.T.Emery, A.D.Bacher, C.Olmer, M.A.Grimm, M.L.Whiten Neutron Transition Densities from 88Sr(p, p') at E(p) = 200 MeV NUCLEAR REACTIONS 88Sr(polarized p, p'), (polarized p, p), E=200 MeV; measured σ(θ), analyzing power vs θ. 88Sr levels deduced neutron transition densities. Shell model comparison.
doi: 10.1103/PhysRevC.47.2146
1992BA27 Phys.Rev. C45, 3000 (1992) J(π) Composition of the Spin-Dipole Resonance in 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319, 800 MeV; analyzed data; deduced transverse isovector NN-t-matrix amplitude energy dependence role in J, π interference.
doi: 10.1103/PhysRevC.45.3000
1992MO17 Phys.Rev. C46, 1008 (1992) M.Morlet, E.Tomasi-Gustafsson, A.Willis, J.Van de Wiele, N.Marty, C.Glashausser, B.N.Johnson, F.T.Baker, D.Beatty, L.Bimbot, C.Djalali, G.W.R.Edwards, A.Green, J.Guillot, F.Jourdan, H.Langevin-Joliot, L.Rosier, M.Y.Youn Isoscalar Spin Excitation in 40Ca NUCLEAR REACTIONS 40Ca(polarized d, d'), E=400 MeV; measured spin transfer parameters analyzing powers, polarizing power. 40Ca deduced isoscalar spin strength distribution. Reanalyzed 12C(polarized d, d') data.
doi: 10.1103/PhysRevC.46.1008
1991BA26 Phys.Rev. C44, 93 (1991) F.T.Baker, L.Bimbot, R.W.Fergerson, C.Glashausser, A.Green, O.Hausser, K.Hicks, K.Jones, C.A.Miller, M.Vetterli, R.Abegg, D.Beatty, B.Bonin, B.Castel, X.Y.Chen, V.Cupps, C.Djalali, R.Henderson, K.P.Jackson, R.Jeppesen, K.Nakayama, S.K.Nanda, R.Sawafta, S.Yen Spin Decomposition of the Responses of 44Ca and 48Ca to 300 MeV Protons NUCLEAR REACTIONS 44Ca(polarized p, p'), E=290 MeV; 48Ca(polarized p, p'), E=318 MeV; measured σ(θ, Ep), analyzing power, spin-flip σ(θ). 44,48Ca deduced giant, spin resonance strength distributions.
doi: 10.1103/PhysRevC.44.93
1991CH32 Phys.Rev.Lett. 67, 1982 (1991) J.Chiba, T.Kobayashi, T.Nagae, I.Arai, N.Kato, H.Kitayama, A.Manabe, M.Tanaka, M.Tomizawa, D.Beatty, G.Edwards, C.Glashausser, G.J.Kumbartzki, R.D.Ransome, F.T.Baker Coincidence Measurements of (p, n) Reactions at 1.5 GeV/c on C and H in the Δ Excitation Region NUCLEAR REACTIONS C, 1H(p, n), E at 1.5 GeV/c; measured σ(θ) vs neutron momentum; deduced isobar peak location features.
doi: 10.1103/PhysRevLett.67.1982
1991HA01 Phys.Rev. C43, 230 (1991) O.Hausser, M.C.Vetterli, R.W.Fergerson, C.Glashausser, R.C.Jeppesen, R.D.Smith, R.Abegg, F.T.Baker, A.Celler, R.L.Helmer, R.Henderson, K.Hicks, M.J.Iqbal, K.P.Jackson, K.W.Jones, J.Lisantti, J.Mildenberger, C.A.Miller, R.S.Sawafta, S.Yen Nuclear Response in the 54Fe(p(pol), p(pol)') Reaction at 290 MeV NUCLEAR REACTIONS 54Fe(polarized p, p'), E=290 MeV; measured σ(θ), spin observables, analyzing power, spin-flip probabilities. 54Fe(n, p), E=298 MeV; analyzed data. 54Fe deduced isovector giant dipole, isoscalar giant quadrupole resonance. 54Mn deduced Gamow-Teller transition strength, quenching. Surface RPA model.
doi: 10.1103/PhysRevC.43.230
1990BA14 Phys.Lett. 237B, 337 (1990) F.T.Baker, L.Bimbot, B.Castel, R.W.Fergerson, C.Glashausser, A.Green, O.Hausser, K.Hicks, K.Jones, C.A.Miller, S.K.Nanda, R.D.Smith, M.Vetterli, J.Wambach, R.Abegg, D.Beatty, V.Cupps, C.Djalali, R.Henderson, K.P.Jackson, R.Jeppesen, J.Lisantti, M.Morlet, R.Sawafta, W.Unkelbach, A.Willis, S.Yen The Nuclear Spin Response to Intermediate Energy Protons NUCLEAR REACTIONS 12C, 90Zr, 40,44,48Ca, 24Mg, 54Fe(polarized p, p'), E ≈ 300 MeV; 40Ca(polarized p, p'), E=800 MeV; measured spin-flip transition probability; deduced enhanced spin response features. Continuum RPA.
doi: 10.1016/0370-2693(90)91185-E
1990BA61 J.Phys.(Paris), Colloq.C-6, 185 (1990) Spin/Isospin/Multipole Response of the Nuclear Continuum using Hadron Scattering NUCLEAR REACTIONS 12C, 40,44,48Ca, 54Fe, 208Pb(p, p'), (polarized p, p'), E=200-800 MeV; compiled data analyses. 12C(polarized d, d'), E=400 MeV; measured deuteron spectra; deduced ΔS=0 transition suppression, no evidence for isovector transition.
1990BI09 Phys.Rev. C42, 2367 (1990) L.Bimbot, R.W.Fergerson, C.Glashausser, K.W.Jones, F.T.Baker, D.Beatty, V.Cupps, A.Green, S.Nanda Nuclear Spin Response of 40Ca to 800 MeV Polarized Protons NUCLEAR REACTIONS 40Ca(polarized p, p'), E=800 MeV; measured missing mass spectra, σ(θ, Ep), spin-flip probability; deduced reaction mechanism. 40Ca deduced nuclear spin response.
doi: 10.1103/PhysRevC.42.2367
1990MO29 Phys.Lett. 247B, 228 (1990) M.Morlet, A.Willis, J.Van de Wiele, N.Marty, J.Guillot, H.Langevin-Joliot, L.Bimbot, L.Rosier, E.Tomasi-Gustafsson, G.W.R.Edwards, R.W.Fergerson, C.Glashausser, D.Beatty, A.Green, C.Djalali, F.T.Baker, J.C.Duchazeaubeneix Signatures for Isoscalar Spin Transitions Excited in (d(pol), d(pol)') Reactions NUCLEAR REACTIONS 12C(polarized d, d'), E=400 MeV; measured polarization observables. 12C deduced isoscalar spin transition signatures.
doi: 10.1016/0370-2693(90)90887-C
1990MO38 J.Phys.(Paris), Colloq.C-6, 599 (1990) M.Morlet, A.Willis, J.van de Wiele, N.Marty, J.Guillot, H.Langevin-Joliot, L.Bimbot, L.Rosier, C.Djalali, E.Tomasi-Gustafsson, G.W.R.Edwards, R.W.Fergerson, C.Glashausser, D.Beatty, A.Green, F.T.Baker A Signature for Isoscalar-Spin Transitions in (d(pol), d(pol)') Scattering NUCLEAR REACTIONS 12C(polarized d, d'), E=400 MeV; measured σ(Ed'); deduced isoscalar spin transition signatures.
1990SE13 Nucl.Phys. A518, 536 (1990) A.Sethi, F.T.Baker, G.T.Emery, W.P.Jones, M.A.Grimm, Jr. 194,198Pt(p(pol), p') Reaction and the Interacting Boson Model NUCLEAR REACTIONS 194,198Pt(polarized p, p'), E=135 MeV; measured σ(θ, Ep'), analyzing power vs θ, Ep'. 194,198Pt levels deduced matrix elements. Coupled channels calculations, interacting boson model analysis with, without a g-boson. Polarized protons, enriched targets.
doi: 10.1016/0375-9474(90)90145-C
1989BA54 Nucl.Phys. A501, 546 (1989) F.T.Baker, A.Sethi, V.Penumetcha, G.T.Emery, W.P.Jones, M.A.Grimm, M.L.Whiten 192Os(p(pol), p') Reaction at 135 MeV NUCLEAR REACTIONS 192Os(polarized p, p'), E=134.5 MeV; measured σ(θ), analyzing power vs θ; deduced matrix elements for excitation of 4+ states. 192Os levels deduced deformation lengths. Enriched target. Coupled-channels analysis.
doi: 10.1016/0375-9474(89)90147-4
1989BA55 Phys.Rev. C40, 1877 (1989) F.T.Baker, L.Bimbot, R.W.Fergerson, C.Glashausser, A.Green, K.Jones, W.G.Love, S.Nanda Spin Dipole and Quadrupole Resonances in 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319 MeV; measured absolute σ(θ). 40Ca deduced spin quadrupole resonance, spin-dipole strength distribution.
doi: 10.1103/PhysRevC.40.1877
1988BA06 Phys.Rev. C37, 1350 (1988) F.T.Baker, L.Bimbot, R.W.Fergerson, C.Glashausser, K.Jones, A.Green, K.Nakayama, S.Nanda Using the (p(pol), p(pol)') Reaction to Study ΔS = 0 Giant Resonances NUCLEAR REACTIONS 40Ca(polarized p, p'), E=318 MeV; measured σ(θp', Ep'). 40Ca deduced ΔS=0 multipole transition strength distribution, EWSR.
doi: 10.1103/PhysRevC.37.1350
1987GL02 Phys.Rev.Lett. 58, 2404 (1987) C.Glashausser, K.Jones, F.T.Baker, L.Bimbot, H.Esbensen, R.W.Fergerson, A.Green, S.Nanda, R.D.Smith Enhancement of the Relative (ΔS = 1)/(ΔS = 0) Response of 40Ca at High Excitation Energies NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319 MeV; measured σ(Ep', θp'), spin-flip probabilities, σ vs excitation energy. 40Ca deduced nuclear response function vs excitation energy. Focal-plane polarimeter. Espensen-Bertsch slab response model.
doi: 10.1103/PhysRevLett.58.2404
1985BA53 Phys.Rev. C32, 1430 (1985) E4 Systematics and the Interacting-Boson Model NUCLEAR STRUCTURE A=155-190; calculated E2, E4 transition reduced matrix elements; analyzed systematics; deduced g-boson inclusion necessity. Interacting boson model.
doi: 10.1103/PhysRevC.32.1430
1985BA64 Phys.Rev. C32, 2212 (1985) F.T.Baker, A.Sethi, V.Penumetcha, G.T.Emery, W.P.Jones, M.A.Grimm, M.L.Whiten g Bosons and the Third 4+ State in 192Os NUCLEAR REACTIONS 192Os(polarized p, p'), E=135 MeV; measured σ(Ep'), σ(θ). 192Os deduced 4+ states, reduced matrix elements, intruder characteristics.
doi: 10.1103/PhysRevC.32.2212
1984GR02 Phys.Rev. C29, 459 (1984) E.E.Gross, T.P.Cleary, J.L.C.Ford, Jr., D.C.Hensley, K.S.Toth, F.T.Baker, A.Scott, C.R.Bingham, J.A.Vrba Nuclear Moments of the First Excited State of 22Ne from 22Ne(132 MeV) + 208Pb Scattering NUCLEAR REACTIONS 208Pb(22Ne, 22Ne), (22Ne, 22Ne'), E=132 MeV; measured σ(θ); deduced optical potential parameters. 22Ne levels deduced quadrupole, hexadecapole deformation parameters, transition matrix elements. Enriched target, coupled-channels analysis.
doi: 10.1103/PhysRevC.29.459
1983BA06 Nucl.Phys. A393, 283 (1983) F.T.Baker, A.Scott, M.A.Grimm, W.G.Love, V.Penumetcha, C.Glashausser, G.S.Adams, G.Igo, G.W.Hoffmann, J.M.Moss, W.Swenson, B.E.Wood The 90,92Zr(p(pol), p') Reactions at E(p) = 800 MeV NUCLEAR REACTIONS 90,92Zr(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(Ep', θ), σ(θ), Aθ, A(Ep', θ). Distorted wave analyses, collective, semimicroscopic-models, free nucleon-nucleon t-matrix. Enriched targets.
doi: 10.1016/0375-9474(83)90143-4
1982BA38 Nucl.Phys. A386, 45 (1982) F.T.Baker, A.Scott, W.G.Love, J.A.Mowrey, W.P.Jones, J.D.Wiggins A Comparison of t-Matrix and G-Matrix Analyses for the 207Pb(p, p') Reaction at E(p) = 95 MeV NUCLEAR REACTIONS 207Pb(p, p'), E=95 MeV; measured σ(Ep', θ). 207Pb deduced levels, β(L). Semi-microscopic DWBA, DWIA calculations.
doi: 10.1016/0375-9474(82)90400-6
1982GL08 Phys.Lett. 116B, 215 (1982) C.Glashausser, R.De Swiniarski, K.Jones, S.Nanda, F.T.Baker, M.Grimm, V.Penumetcha, A.Scott, G.Adams, G.Igo, G.W.Hoffmann, J.Moss, W.Swenson, B.E.Wood Coupled-Channels Analysis of 800 MeV Polarized Proton Inelastic Scattering from 18O NUCLEAR REACTIONS 18O(polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 18O deduced β2, β4, β6. Coupled-channels analysis.
doi: 10.1016/0370-2693(82)90328-8
1981BA01 Nucl.Phys. A351, 63 (1981) F.T.Baker, A.Scott, R.C.Styles, T.H.Kruse, K.Jones, R.Suchannek 182,184,186W(α, α') Reactions at Eα = 24 MeV NUCLEAR REACTIONS 182,184,186W(α, α'), E=24 MeV; measured σ(Eα', θ); deduced optical model parameters. 182,184,186W deduced β2, β4 charge, density quadrupole, hexadecapole moments. 184W deduced β3. Enriched targets. Rotational-vibrational model.
doi: 10.1016/0375-9474(81)90545-5
1981BA49 Nucl.Phys. A371, 68 (1981) F.T.Baker, M.A.Grimm, Jr., A.Scott, R.C.Styles, T.H.Kruse, K.Jones, R.Suchannek 192Os(α, α') Reaction at Eα = 24 MeV and the IBA Model NUCLEAR REACTIONS 192Os(α, α), (α, α'), E=24 MeV; measured σ(θ), σ(Eα', θ). 192Os deduced B(E4), deformation parameter β4. Enriched target. Interacting boson model, coupled-channels analysis.
doi: 10.1016/0375-9474(81)90745-4
1981BA54 Phys.Rev.Lett. 47, 1823 (1981) F.T.Baker, C.Glashausser, A.Scott, M.A.Grimm, G.S.Adams, G.Hoffmann, G.Igo, W.G.Love, J.M.Moss, S.Nanda, V.Penumetcha, W.Swenson, B.E.Wood Test of Data-to-Data Relations for the Reactions 90,92Zr(p(pol), p') at 800 MeV NUCLEAR REACTIONS 90,92Zr(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced data-to-data relation inadequacies.
doi: 10.1103/PhysRevLett.47.1823
1981SC04 Nucl.Phys. A357, 9 (1981) A.Scott, F.T.Baker, W.G.Love, J.D.Wiggins, Jr., M.L.Whiten Comparison of the 92Mo(p, p') and 90Zr(p, p') Reactions at 61.2 MeV NUCLEAR REACTIONS 92Mo(p, p'), E=61.2 MeV; measured σ(Ep', θ). 90Zr(p, p'), E=61.2 MeV; analyzed σ(θ). 92Mo deduced levels, deformation parameter β(L). Isotopically enriched target.
doi: 10.1016/0375-9474(81)90623-0
1981SC11 Nucl.Phys. A366, 91 (1981) A.Scott, F.T.Baker, W.G.Love, W.P.Jones, J.D.Wiggins, Jr. 207Pb(p, p') Measurements at 135 and 61 MeV, the Effective Interaction and Core Polarization NUCLEAR REACTIONS 207Pb(p, p'), E=134.8 MeV; measured σ(Ep', θ). 207Pb deduced levels, deformation β(L). Enriched target. Microscopic DWBA, DWIA calculations.
doi: 10.1016/0375-9474(81)90489-9
1980MO06 Phys.Rev.Lett. 44, 1189 (1980) J.M.Moss, C.Glashausser, F.T.Baker, R.Boudrie, W.D.Cornelius, N.Hintz, G.Hoffmann, G.Kyle, W.G.Love, A.Scott, H.A.Thiessen Excitation of Unnatural-Parity States in 12C by 800-MeV Polarized Protons NUCLEAR REACTIONS 12C(polarized p, p'), E=800 MeV; measured σ(θ), A(θ). 12C levels deduced T, J, π. DWIA analysis.
doi: 10.1103/PhysRevLett.44.1189
1980SC21 Phys.Rev.Lett. 45, 1315 (1980) A.Scott, F.T.Baker, M.A.Grimm, Jr., J.H.Johnson, V.Penumetcha, R.C.Styles, W.G.Love, W.P.Jones, J.D.Wiggins, Jr. Shapes of Measured (p(pol), p') Analyzing Powers at 160 MeV for Proton States in 90Zr and Neutron States in 92Zr NUCLEAR REACTIONS 90,92Zr(polarized p, p'), E=160 MeV; measured analyzing power vs θ; deduced spin-orbit potential parameters. 90,92Zr levels deduced configurations, β. DWIA, free nucleon-nucleon t-matrix.
doi: 10.1103/PhysRevLett.45.1315
1979BA19 Nucl.Phys. A321, 222 (1979) F.T.Baker, A.Scott, T.P.Cleary, J.L.C.Ford, E.E.Gross, D.C.Hensley 194Pt(12C, 12C') Reaction and the Triaxial-Rotor Model NUCLEAR REACTIONS 194Pt(12C, 12C'), E=78 MeV, θ(cm)=25°-80°; measured σ(E(12C), θcm). 194Pt deduced optical-model parameters, asymmetric-rotor model parameters β2, β4, γ. Enriched target.
doi: 10.1016/0375-9474(79)90695-X
1979BA21 Phys.Rev.Lett. 43, 195 (1979) Possible Origin of the 'Anomalous' Interference Terms in 192,194Pt NUCLEAR STRUCTURE 194Pt; calculated E2 matrix elements; deduced β2, β4, γ parameters. Rigid asymmetric model.
doi: 10.1103/PhysRevLett.43.195
1979BA32 Nucl.Phys. A325, 525 (1979) F.T.Baker, A.Scott, E.E.Gross, D.C.Hensley, D.L.Hillis 30Si(12C, 12C') Reaction at 41.3 MeV NUCLEAR REACTIONS 30Si(12C, 12C'), E=41.3 MeV; measured σ(E(12C'), θ); deduced optical-model parameters. 30Si level deduced sign, magnitude of nuclear β. Enriched target.
doi: 10.1016/0375-9474(79)90030-7
1979BA39 Nucl.Phys. A331, 39 (1979) A New Rigid Asymmetric-Rotor Model Description of the Heavy Transitional Nuclei NUCLEAR STRUCTURE 184,186W, 186,188,190,192Os, 192,194,196Pt, 198,200Hg; calculated E2, E4 properties. Davydov-Filippov asymmetric rotor model, hexadecapole shape components.
doi: 10.1016/0375-9474(79)90299-9
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
1978BA24 Nucl.Phys. A299, 357 (1978) Heavy-Ion Excitation of 3- States in Deformed Nuclei NUCLEAR STRUCTURE 148,150Nd; reanalyzed data; calculated matrix elements.
doi: 10.1016/0375-9474(78)90036-2
1978LO01 Phys.Lett. 73B, 277 (1978) W.G.Love, A.Scott, F.T.Baker, W.P.Jones, J.D.Wiggins, Jr. A Test of the DWIA at 135 MeV Using the 207Pb(p, p') Reaction NUCLEAR REACTIONS 207Pb(p, p'), E=135 MeV; calculted σ(θ).
doi: 10.1016/0370-2693(78)90513-0
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
1977BA31 Nucl.Phys. A284, 135 (1977) F.T.Baker, A.Scott, E.E.Gross, D.C.Hensley, D.L.Hillis Nuclear Reorientation Effects for the 26Mg, 28Si(12C, 12C') Reactions at E = 41 MeV NUCLEAR REACTIONS 26Mg(12C, 12C'), E=41.3 MeV, θ(cm)=19°-66°; 28Si(12C, 12C'), E=41.4 MeV, θ(cm)=18°-70°; measured σ(E(12C'), θ(cm)). 26Mg, 28Si deduced optical-model parameters, nuclear β2 deformations, signs of 2+ quadrupole moments. Enriched targets.
doi: 10.1016/0375-9474(77)90690-X
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
1977EC03 Phys.Rev. C16, 1020 (1977) J.S.Eck, D.O.Elliott, W.J.Thompson, F.T.Baker Nuclear Shapes of 24Mg and 28Si by Inelastic Scattering of 12C and 16,18O NUCLEAR REACTIONS 28Si, 24Mg(12C, 12C), (12C, 12C'), E=25, 30 MeV; 24Mg(16O, 16O), (16O, 16O'), 28Si(18O, 18O), (18O, 18O'), E=36 MeV; 28Si(16O, 16O), (16O, 16O'), E=33, 36, 38 MeV; measured σ(θ); deduced optical model parameters. 24Mg, 28Si deduced β.
doi: 10.1103/PhysRevC.16.1020
1977HI07 Phys.Rev. C16, 1467 (1977) D.L.Hillis, E.E.Gross, D.C.Hensley, C.R.Bingham, F.T.Baker, A.Scott Multistep Effects in the Elastic and Inelastic Scattering of 70.4-MeV 12C Ions from the Even Neodymium Isotopes NUCLEAR REACTIONS 142,144,146,148,150Nd(12C, 12C), (12C, 12C'), E=70.4 MeV; measured σ(θ); deduced optical model parameters. 142,144,146,148,150Nd deduced β. Coupled-channel analysis. Enriched targets.
doi: 10.1103/PhysRevC.16.1467
1976BA06 Nucl.Phys. A258, 43 (1976) F.T.Baker, T.H.Kruse, W.Hartwig, I.Y.Lee, J.X.Saladin Nuclear Shapes of the Transitional Nuclei 186,188,190,192Os NUCLEAR REACTIONS 186,188,190,192Os(α, α'), E=13-24 MeV, θlab=130°; measured σ(E, Eα'). 186,188,190,192Os deduced β2 charge, mass deformations, 186,188,192Os deduced β4 charge, mass deformations. 192Os(α, α'), E=24 MeV; measured σ(Eα', θ). 192Os deduced optical model parameters. Enriched targets.
doi: 10.1016/0375-9474(76)90526-1
1976BA09 Phys.Rev.Lett. 36, 852 (1976) Effect of β4 Deformations on Decoupled Rotational Bands in Odd-A Nuclei NUCLEAR STRUCTURE 187Ir; calculated levels, β.
doi: 10.1103/PhysRevLett.36.852
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
1976HI01 Phys.Rev.Lett. 36, 304 (1976) D.L.Hillis, E.E.Gross, D.C.Hensley, L.D.Rickertsen, C.R.Bingham, A.Scott, F.T.Baker Multistep Processes in the Inelastic Scattering of 70.4-MeV 12C from 144Nd NUCLEAR REACTIONS 144Nd(12C, 12C'), E=70.4 MeV; measured σ(E(12C'), θ). 144Nd levels deduced J, π, coupling.
doi: 10.1103/PhysRevLett.36.304
1975BA03 Phys.Rev. C11, 262 (1975) F.T.Baker, W.Hartwig, T.H.Kruse, E.Ventura Coulomb-Nuclear Interference for the (d, d') Reaction on Isotopes of Nd NUCLEAR REACTIONS 142,144,146,148,150Nd(d, d'), E=5-16 MeV; measured σ(E, Ed'); deduced deformation parameters β2. Enriched targets.
doi: 10.1103/PhysRevC.11.262
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
1975BA30 Phys.Rev.Lett. 35, 469 (1975) E2-E4 Interference for (α, α') Reactions NUCLEAR REACTIONS 184W(α, α'), E=20 MeV; calculated E2/E4 interference in σ.
doi: 10.1103/PhysRevLett.35.469
1975BA41 Nucl.Phys. A250, 79 (1975) F.T.Baker, S.Davis, C.Glashausser, A.B.Robbins Elastic and Inelastic Scattering of 15 MeV Polarized Deuterons from Isotopes of Ca, Cu, Sr, Zr, and Mo NUCLEAR REACTIONS 48Ca, 63Cu, 88Sr, 90,92Zr, 92Mo(polarized d, d), (polarized d, d'), E=15 MeV; measured σ(θ), iT11(θ); deduced optical model parameters. 48Ca, 88Sr, 90,92Zr, 92Mo levels deduced deformation parameters β(L). 92Zr(d, d), E=15 MeV; measured T20(θ), T22(θ). Enriched targets.
doi: 10.1016/0375-9474(75)90201-8
1975BA64 Nucl.Phys. A253, 461 (1975) F.T.Baker, C.Glashausser, A.B.Robbins, E.Ventura Coupled-Channels Effects for Inelastic Scattering of 15 MeV Polarized Deuterons from Ti and Sm Isotopes NUCLEAR REACTIONS 148,152Sm(polarized d, d), (polarized d, d'), E=15 MeV; measured σ(θ), iT11(θ). 48,50Ti, 148,152Sm(polarized d, d), (polarized d, d'), E=15 MeV; deduced optical model parameters. 48,50Ti, 148,152Sm deduced deformation parameters β2. Enriched targets.
doi: 10.1016/0375-9474(75)90492-3
1975GL06 Phys.Rev.Lett. 35, 494 (1975) C.Glashausser, A.B.Robbins, E.Ventura, F.T.Baker, J.Eng, R.Kaita Evidence for Intermediate Structure in the Inelastic Scattering of Polarized Protons from 26Mg and 27Al NUCLEAR REACTIONS 26Mg(polarized p, p'), E=5.5-9.4 MeV; 27Al(polarized p, p), E=6.1-12.0 MeV; measured A(E, θ).
doi: 10.1103/PhysRevLett.35.494
1975LO07 Phys.Rev.Lett. 35, 1219 (1975) Final-State Spin Dependence for Inelastic Scattering from Odd-A Nuclei NUCLEAR REACTIONS 63Cu(polarized p, p), (polarized d, d); calculated σ(θ), A(θ).
doi: 10.1103/PhysRevLett.35.1219
1974BA74 Nucl.Phys. A233, 409 (1974) F.T.Baker, S.Davis, C.Glashausser, A.B.Robbins Elastic and Inelastic Scattering of 15 MeV Polarized Deuterons from Ti, Cr, Fe and Ni Isotopes NUCLEAR REACTIONS 48,50Ti, 52Cr, 54,56Fe, 58,60,62,64Ni(polarized d, d), (polarized d, d'), E=15 MeV; measured σ(θ), iT11(θ); deduced optical model parameters. 48,50Ti, 52Cr, 54,56Fe, 58,60,62,64Ni levels deduced deformation parameters β(L). 54,56Fe, 62Ni(polarized d, d), (polarized d, d'), E=15 MeV; measured t20(θ), t22(θ). 54,56Fe(polarized d, d), (polarized d, d'), E=15 MeV; measured t21(θ). Enriched targets.
doi: 10.1016/0375-9474(74)90466-7
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
1973BA28 Part.Nucl. 5, 29 (1973) F.T.Baker, T.H.Kruse, J.L.Matthews, M.E.Williams 90Zr(d, d') Reaction at E = 15 MeV NUCLEAR REACTIONS 90Zr(d, d'), E=15 MeV; measured σ(θ). Deduced β(L), L.
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
1972BA02 Phys.Rev. C5, 182 (1972) Nuclear Structure of the N = 82 Isotones 140Ce and 139La from the (α, α') Reaction NUCLEAR REACTIONS 140Ce, 139La(α, α), (α, α'), E=45 MeV; measured σ(Eα', θ). 140Ce, 139La deduced levels, J, π, L.
doi: 10.1103/PhysRevC.5.182
1972BA07 Phys.Rev. C5, 544 (1972) 208Pb(3He, 3He') Reaction at 43.7 MeV NUCLEAR REACTIONS 208Pb(3He, 3He'), E=43.7 MeV; measured σ(θ). 208Pb deduced B(EL).
doi: 10.1103/PhysRevC.5.544
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
1970BA19 Phys.Lett. 32B, 47 (1970) Coulomb Excitation by 45 MeV Alpha Particles NUCLEAR REACTIONS 140Ce, 208Pb(α, α'), E=45 MeV; measured σ(θ). 140Ce, 208Pb deduced Coulomb excitation contribution.
doi: 10.1016/0370-2693(70)90334-5
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