NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = E.Rost Found 60 matches. 1994RO09 Phys.Rev. C50, 1729 (1994) Subthreshold Response Function in the Δ-Resonance Region NUCLEAR REACTIONS 16O(e, e'X), E not given; calculated transverse response function; deduced kinematics, Δ mass, width dependences.
doi: 10.1103/PhysRevC.50.1729
1993RO13 Phys.Rev. C47, 2250 (1993) E.Rost, C.E.Price, J.R.Shepard Transverse Response Functions in the Δ-Resonance Region NUCLEAR REACTIONS 12C, 40Ca, 56Fe(e, e'), E not given; calculated transverse response functions. Relativistic Hartree approximation, Δ-resonance.
doi: 10.1103/PhysRevC.47.2250
1992PR01 Phys.Rev. C45, 1089 (1992) C.E.Price, E.Rost, J.R.Shepard, J.A.McNeil Toward a Consistent Random Phase Approximation Based on the Relativistic Hartree Approximation NUCLEAR STRUCTURE 16O, 40Ca; calculated levels, isoscalar transitions. RPA, relativistic Hartree approximation. NUCLEAR REACTIONS 16O, 12C, 40Ca(e, e'), E not given; calculated longitudinal form factor. RPA, relativistic Hartree approximation.
doi: 10.1103/PhysRevC.45.1089
1991KI08 Phys.Rev. C44, 1077 (1991) J.D.King, D.Frekers, R.Abegg, R.E.Azuma, L.Buchmann, C.Chan, T.E.Drake, R.Helmer, K.P.Jackson, L.Lee, C.A.Miller, E.Rost, R.Sawafta, R.Schubank, S.S.M.Wong, S.Yen, X.Q.Zhu Excitation of the 10.957 MeV 0-; T = 0 State in 16O by 400 MeV Protons NUCLEAR REACTIONS 16O(polarized p, p'), E=400 MeV; measured σ(θ), analyzing power vs θ; deduced reaction mechanism.
doi: 10.1103/PhysRevC.44.1077
1991OD03 Phys.Rev. C44, 2426 (1991) J.M.O'Donnell, H.T.Fortune, E.Rost 0+ and 2+ Strengths in Pion Double Charge Exchange to Double Giant-Dipole Resonances NUCLEAR REACTIONS 40Ca(π+, π-), E=165-300 MeV; calculated σ(θ). 40Ca deduced β. Coupled-channels optical model.
doi: 10.1103/PhysRevC.44.2426
1990PI06 Phys.Rev. C41, 2277 (1990) J.Piekarewicz, E.Rost, J.R.Shepard Correlation Observables in (p, p'γ) Reactions NUCLEAR REACTIONS 12C(polarized p, p'γ), E=400 MeV; calculated σ(θp, θγ), analyzing powers vs θ. Relativistic impulse approximation.
doi: 10.1103/PhysRevC.41.2277
1989MC05 Phys.Rev. C40, 399 (1989) J.A.McNeil, R.J.Furnstahl, E.Rost, J.R.Shepard Finite Nucleus Dirac Mean Field Theory and Random Phase Approximation using Finite B Splines NUCLEAR STRUCTURE 16O, 40Ca; calculated levels, isoscalar longitudinal form factors. Finite nucleus Dirac mean field theory.
doi: 10.1103/PhysRevC.40.399
1989RO13 Phys.Rev. C40, 1736 (1989) Dirac Random-Phase-Approximation Analysis of the Inelastic Scattering of 500 MeV Protons from 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=500 MeV; calculated σ(θ), analyzing power, spin transfer observables vs θ. Dirac RPA.
doi: 10.1103/PhysRevC.40.1736
1989SH27 Phys.Rev. C40, 2320 (1989) J.R.Shepard, E.Rost, J.A.McNeil Nonspectral Dirac Random-Phase Approximation for Finite Nuclei NUCLEAR REACTIONS 12C, 16O, 48,40Ca(e, e'), E not given; calculated form factors. Nonspectral Dirac RPA. NUCLEAR STRUCTURE 16O; calculated lowest 1-, T=0 level B(E1). RPA.
doi: 10.1103/PhysRevC.40.2320
1988HI09 Phys.Rev. C38, 229 (1988) K.H.Hicks, R.G.Jeppesen, C.C.K.Lin, R.Abegg, K.P.Jackson, O.Hausser, J.Lisantti, C.A.Miller, E.Rost, R.Sawafta, M.C.Vetterli, S.Yen Inelastic Proton Scattering at 200 to 400 MeV for 24Mg and 28Si in a Microscopic Framework NUCLEAR REACTIONS 12C, 24Mg, 28Si(polarized p, p'), E=200-400 MeV; measured σ(θ), A(θ) vs E; deduced model validity. Relativistic, nonrelativistic DWIA.
doi: 10.1103/PhysRevC.38.229
1988KU27 J.Phys.(London) G14, L253 (1988) Relativistic Suppression Factors in (p, d) Reaction Calculations NUCLEAR REACTIONS 40Ca(p, d), E=120 MeV; calculated Darwin, pseudovector suppression factors vs radius. Relativistic approach.
doi: 10.1088/0305-4616/14/3/002
1988MC03 Phys.Rev.Lett. 61, 814 (1988) J.P.McDermott, E.Rost, J.R.Shepard, C.Y.Cheung Relativistic (γ, p) Calculations at Intermediate Energies NUCLEAR REACTIONS 16O(γ, p), E=196 MeV; 40Ca(γ, p), E=100-300 MeV; calculated σ(θ).
doi: 10.1103/PhysRevLett.61.814
1988SH07 Phys.Rev. C37, 1130 (1988) J.R.Shepard, E.Rost, C.-Y.Cheung, J.A.McNeil Magnetic Response of Closed-Shell ±1 Nuclei in Dirac-Hartree Approximation NUCLEAR REACTIONS 15N(e, e), E not given; calculated isoscalar M1 form factor. Dirac-Hartree approximation. NUCLEAR STRUCTURE 15N, 15O; A=15, 17, 39, 41; calculated μ. Dirac-Hartree approximation.
doi: 10.1103/PhysRevC.37.1130
1987FR05 Phys.Rev. C35, 2236 (1987) D.Frekers, S.S.M.Wong, R.E.Azuma, T.E.Drake, J.D.King, R.Abegg, K.P.Jackson, C.A.Miller, S.Yen, W.P.Alford, R.L.Helmer, C.Broude, S.Mattsson, E.Rost Elastic and Inelastic Scattering of 362 MeV polarized Protons from 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=362 MeV; measured σ(θ), analyzing power. Magnetic spectrometer. Model calculations.
doi: 10.1103/PhysRevC.35.2236
1987RO02 Phys.Rev. C35, 681 (1987) Nucleon-Nucleus Inelastic Scattering using a Relativistic Impulse Approximation with Exchange NUCLEAR REACTIONS 12C(p, p'), (polarized p, p'), E=135, 200, 400 MeV; calculated σ(θ), analyzing powers. Relativistic impulse approximation, exchange.
doi: 10.1103/PhysRevC.35.681
1986SH01 Phys.Rev. C33, 634 (1986) J.R.Shepard, E.Rost, J.A.McNeil Relativistic Plane-Wave Impulse Approximation for Nuclear Inelastic Scattering of Protons and Electrons NUCLEAR REACTIONS 12C(e, e'), E not given; 12C(p, p'), E=150 MeV; calculated nuclear transition densities, currents. 12C levels deduced structure information. Relativistic plane-wave impulse approximation.
doi: 10.1103/PhysRevC.33.634
1985SP03 Phys.Rev.Lett. 54, 2207 (1985) D.A.Sparrow, J.Piekarewicz, E.Rost, J.R.Shepard, J.A.McNeil, T.A.Carey, J.B.McClelland Relativistic Impulse Approximation, Nuclear Currents, and the Spin-Difference Function NUCLEAR REACTIONS 12C(p, p'), E=150 MeV; calculated P(θ), analyzing power vs θ difference; deduced nuclear currents role. Relativistic approximation.
doi: 10.1103/PhysRevLett.54.2207
1984RO02 Phys.Rev. C29, 209 (1984) E.Rost, J.R.Shepard, E.R.Siciliano, J.A.McNeil Impulse Approximation Dirac Theory of Inelastic Proton Nucleus Collective Excitations NUCLEAR REACTIONS 54Fe(polarized p, p), E=800 MeV; calculated σ(θ), analyzing power vs θ. Dirac theory, impulse approximation.
doi: 10.1103/PhysRevC.29.209
1984SH08 Phys.Rev. C29, 2243 (1984) J.R.Shepard, E.Rost, E.R.Siciliano, J.A.McNeil Dirac Single-Particle Wave Functions in Inelastic Electron Scattering NUCLEAR REACTIONS 12C(e, e), (e, e'), E not given; calculated charge, transverse form factors; deduced transverse isoscalar transition linear inelastic amplitude role. Dirac single particle wave functions.
doi: 10.1103/PhysRevC.29.2243
1984SH21 Phys.Rev. C30, 1604 (1984) J.R.Shepard, E.Rost, J.Piekarewicz Microscopic Relativistic Nucleon-Nucleus Inelastic Scattering NUCLEAR REACTIONS 12C(p, p'), E not given; calculated natural, unnatural parity level amplitudes. Relativistic treatment.
doi: 10.1103/PhysRevC.30.1604
1982RO09 Phys.Rev.Lett. 49, 448 (1982) E.Rost, J.R.Shepard, D.Murdock Dirac Wave Functions in Nuclear Distorted-Wave Calculations NUCLEAR REACTIONS 90Zr(p, n), E=80 MeV; calculated σ(θ), analyzing power vs θ. Distorted waves, Dirac, Schrodinger approaches.
doi: 10.1103/PhysRevLett.49.448
1982SH03 Phys.Rev. C25, 1127 (1982) Failure of the Distorted-Wave Born Approximation in Analysis of the 24Mg(p(pol), d)23Mg Reaction at T(p) = 94 MeV NUCLEAR REACTIONS 24Mg(polarized p, d), E=94 MeV; calculated σ(θ), analyzing power vs θ; deduced DWBA inadequacy. DWBA, CCBA, exact finite-range effects, deuteron tensor interaction, breakup, multi-step process, radial cutoff.
doi: 10.1103/PhysRevC.25.1127
1982SH06 Phys.Rev. C25, 2660 (1982) Analytic Eikonal Model for Intermediate Energy Stripping and Pickup Reactions NUCLEAR REACTIONS 16O(d, p), E=400, 660 MeV; 12C(p, d), E=800 MeV; calculated σ(θ). Eikonal model.
doi: 10.1103/PhysRevC.25.2660
1982SH11 Phys.Rev.Lett. 49, 14 (1982) J.R.Shepard, E.Rost, D.Murdock Dirac Phenomenology for Deuteron Elastic Scattering NUCLEAR REACTIONS 58Ni(d, d), (polarized d, d), E=80 MeV; analyzed σ(θ), vector analyzing power vs θ; deduced effective central potential. Dirac, Schrodinger equation approaches.
doi: 10.1103/PhysRevLett.49.14
1981WE03 Nucl.Phys. A355, 45 (1981) R.C.Weiss, R.E.Anderson, J.J.Kraushaar, R.A.Ristinen, E.Rost, S.Shastry A Study of Particle-Vibration Multiplets in 203Tl using the 205Tl(p, t)203Tl, 208Pb(p, t)206Pb and 206Pb(p, t)204Pb Reactions NUCLEAR REACTIONS 205Tl, 206,208Pb(p, t), E=26.2 MeV; measured σ(θ, Et). 203Tl deduced levels, L, J, π. 203Tl, 204,206Pb levels deduced L=0, 2 enhancement factors, J, π. DWBA analysis, intermediate coupling wave functions.
doi: 10.1016/0375-9474(81)90131-7
1980BA45 Phys.Lett. B97, 45 (1980) B.M.Barnett, W.Gyles, R.R.Johnson, K.L.Erdman, J.Johnstone, J.J.Kraushaar, S.Lepp, T.G.Masterson, E.Rost, D.R.Gill, A.W.Thomas, J.Alster, I.Navon, R.H.Landau Proton Radii Determinations from the Ratio of π+ Elastic Scattering from 11B and 12C NUCLEAR REACTIONS 12C, 11B(π+, π+), E=38.6, 47.7 MeV; measured σ(θ). 12C, 11B deduced rms charge radii differences.
doi: 10.1016/0370-2693(80)90543-2
1979DI01 Phys.Rev. C19, 1132 (1979) N.J.DiGiacomo, R.L.Boudrie, I.Brissaud, J.J.Kraushaar, R.J.Peterson, R.A.Ristinen, E.S.Rost, G.R.Smith Elastic and Inelastic Diffraction Scattering of 0.8 GeV Protons by 89Y and 90Zr NUCLEAR REACTIONS 89Y, 90Zr(p, p'), E=0.8 GeV; measured σ(θ). 89Y, 90Zr levels deduced β(L). Optical model, DWBA analysis.
doi: 10.1103/PhysRevC.19.1132
1979JO08 Phys.Rev.Lett. 43, 844 (1979) R.R.Johnson, T.Masterson, B.Bassalleck, W.Gyles, T.Marks, K.L.Erdman, A.W.Thomas, D.R.Gill, E.Rost, J.J.Kraushaar, J.Alster, C.Sabev, J.Arvieux, M.Krell Neutron Radii Determinations from the Ratio of π- Elastic Scattering From 12,13C and 16,18O NUCLEAR REACTIONS 12,13C(π-, π-), E=29.2-49.5 MeV; 16,18O(π-, π-), E=29.2 MeV; measured σ(θ). 13C, 18O deduced neutron radii relative to 12C, 16O. Optical model analysis.
doi: 10.1103/PhysRevLett.43.844
1979SH21 Phys.Lett. 89B, 13 (1979) J.R.Shepard, E.Rost, G.R.Smith Evidence for Pion Exchange Currents in the Analysis of the 4He(p, d)3He Reaction at Intermediate Energies NUCLEAR REACTIONS 4He(p, d), E=434, 770 MeV; calculated σ(θ). DWBA, no pion exchange currents.
doi: 10.1016/0370-2693(79)90065-0
1978AR16 Nucl.Phys. A312, 368 (1978) J.Arvieux, J.P.Albanese, J.Bolger, E.Boschitz, C.H.Q.Ingram, L.Pflug, J.Jansen, J.Zichy, E.Rost, A.S.Rosenthal Elastic and Inelastic Scattering of π± by 208Pb NUCLEAR REACTIONS 208Pb(π+, π+), E=80, 116 MeV; 208Pb(π-, π-), E=116 MeV; measured σ(θ) for ground state at 80, 116 MeV, for first 3- excited state at 116 MeV. Optical potential, collective model analysis.
doi: 10.1016/0375-9474(78)90597-3
1978RO06 Phys.Rev. C17, 1513 (1978) E.Rost, J.R.Shepard, D.A.Sparrow Distorted-Wave Born-Approximation Description of the 4He(p, d)3He Reaction at E = 770 MeV NUCLEAR REACTIONS 4He(p, d), E=770 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.17.1513
1977DI03 Phys.Lett. 66B, 421 (1977) N.J.Digiacomo, A.S.Rosenthal, E.Rost, D.A.Sparrow Pion-Nucleus Scattering at 50 MeV NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 208Pb(π+, X), (π+, π+), E=50 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(77)90575-5
1977RO25 Phys.Lett. 71B, 237 (1977) A.S.Rosenthal, E.Rost, D.A.Sparrow, N.J.Digiacomo Second Order Density Effects in Low Energy Pion Scattering NUCLEAR REACTIONS 56Fe, 208Pb(π+, π+), E=50 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(77)90202-7
1976IV03 Phys.Rev. C14, 1733 (1976) Pion-Gamma Angular Correlations Following Inelastic Scattering NUCLEAR REACTIONS 12C(π, π'γ), E=30-150 MeV; calculated pion-γ angular correlation.
doi: 10.1103/PhysRevC.14.1733
1975IV05 Phys.Rev. C12, 1589 (1975) Pion Elastic Scattering from Aligned Targets NUCLEAR REACTIONS 165Ho(π, π), E=100-200 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.12.1589
1975RO29 Phys.Lett. 59B, 413 (1975) Exact Finite Range DWBA Results for the 12C(p, d)11C Reaction at 700 MeV NUCLEAR REACTIONS 12C(p, d), E=700 MeV; calculated σ(Ed, θ). DWBA calculation.
doi: 10.1016/0370-2693(75)90332-9
1974BA58 Phys.Lett. 52B, 57 (1974) S.D.Baker, R.Bertini, R.Beurtey, F.Brochard, G.Bruge, H.Catz, A.Chaumeaux, G.Cvijanovich, J.M.Durand, J.C.Faivre, J.M.Fontaine, D.Garreta, F.Hibou, D.Legrand, J.C.Lugol, J.Saudinos, J.Thirion, E.Rost The 12C(p, d)11C Reaction at 700 MeV NUCLEAR REACTIONS 12C(p, d), E=700 MeV; measured σ(Ed, θ). 11C levels deduced reaction mechanism.
doi: 10.1016/0370-2693(74)90718-7
1974GE09 Phys.Lett. 52B, 39 (1974) E.Gerlic, J.Van de Wiele, H.Langevin-Joliot, J.P.Didelez, G.Duhamel, E.Rost The (τ, α) Reaction at 216 MeV NUCLEAR REACTIONS 12C, 16O(3He, α), E=216 MeV; measured σ(Eα, θ). 11C, 15O levels deduced reaction mechanism.
doi: 10.1016/0370-2693(74)90712-6
1974KU17 Phys.Lett. 53B, 9 (1974) On the Analysis of the 12C(d, τ)11B Reaction at 80 MeV NUCLEAR REACTIONS 12C(d, 3He), E=80 MeV; calculated σ(E(3He), θ). 11B deduced β2.
doi: 10.1016/0370-2693(74)90329-3
1973BA13 Ann.Phys.(New York) 76, 437 (1973) H.W.Baer, J.J.Kraushaar, C.E.Moss, N.S.P.King, R.E.L.Green, P.D.Kunz, E.Rost Study of the (p, t) Reaction on the Even-A Titanium Isotopes NUCLEAR REACTIONS 46,48,50Ti(p, t), E=19, 23, 27 MeV; measured σ(Et, θ). Deduced L. 44,46,48Ti deduced levels, J, π.
doi: 10.1016/0003-4916(73)90043-2
1973RO10 Phys.Lett. 43B, 17 (1973) Analysis of (π+, p) and (p, π+) Reactions NUCLEAR REACTIONS 12C(π+, p), (p, π+), E=68, 185 MeV; calculated σ(θ). DWBA.
doi: 10.1016/0370-2693(73)90531-5
1971AB01 Nucl.Phys. A162, 173 (1971) Rotational Levels of Deformed Doubly Even Nuclei NUCLEAR STRUCTURE 158Dy, 164Er, 168Yb, 174Hf; calculated intrinsic, rotational energies.
doi: 10.1016/0375-9474(71)90492-1
1971ED02 Phys.Rev.Lett. 26, 785 (1971) π-Carbon Inelastic Scattering Near the 33 Resonance NUCLEAR REACTIONS 12C(π-, π-'), E=120-280 MeV; calculated σ(θ). 12C deduced deformation parameters. DWBA, Kisslinger optical potential.
doi: 10.1103/PhysRevLett.26.785
1971RO04 Nucl.Phys. A162, 376 (1971) Finite-Range Corrections in Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 48Ti(p, t), E=27 MeV; calculated σ(θ). Finite-range DWBA.
doi: 10.1016/0375-9474(71)90992-4
1971RO12 Phys.Rev. C3, 2491 (1971) Shapes of Angular Distributions of (3He, t) and (p, n) Transitions to 0+ Antianalog States NUCLEAR REACTIONS 40Ar(3He, t), E not given; calculated σ(θ), form factors for antianalog transitions.
doi: 10.1103/PhysRevC.3.2491
1971RO32 Phys.Lett. 37B, 247 (1971) Pion-Nucleus Charge Exchange Scattering at Intermediate Energies NUCLEAR REACTIONS 93Nb(π+, π-), E < 300 MeV; calculated σ(E;θ). Kisslinger optical model.
doi: 10.1016/0370-2693(71)90009-8
1970DE18 Nucl.Phys. A150, 187 (1970) D.W.Devins, M.E.Rickey, S.Hayakawa, E.Rost T = 9/2 Analogue State in 63Ni NUCLEAR REACTIONS 64Ni(p, d), E=27.5 MeV; measured σ(Ed, θ). 63Ni deduced isobaric analog state, S. Enriched target.
doi: 10.1016/0375-9474(70)90465-3
1969HA21 Phys.Letters 29B, 327 (1969) S.I.Hayakawa, J.J.Kraushaar, P.D.Kunz, E.Rost Study of the Effective Two-Body Force Using the 54Fe(3He, t) Charge Exchange Reaction NUCLEAR REACTIONS 54Fe(3He, t), E=37.5 MeV; measured σ(E, θ). Microscopic DWBA analysis.
doi: 10.1016/0370-2693(69)90374-8
1969HA47 Nucl.Phys. A139, 465 (1969) S.I.Hayakawa, W.L.Fadner, J.J.Kraushaar, E.Rost Study of the 90Zr(3He, t) Reaction NUCLEAR REACTIONS 90Zr(3He, t), E=37.7 MeV; measured σ(Et, θ). 90Nb deduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(69)91123-3
1969KU02 Phys.Rev. 177, 1737(1969) Particle Transfer Reactions on Deformed Nuclei NUCLEAR REACTIONS 24Mg(p, p), (p, d), E=27.3 MeV; measured σ(Ed, θ). 23Mg deduced levels. Enriched target, optical-model analysis.
doi: 10.1103/PhysRev.177.1737
1969KU09 Phys.Rev. 185, 1528 (1969) P.D.Kunz, E.Rost, R.R.Johnson, G.D.Jones, S.I.Hayakawa Analyses of Quasielastic and Quasi-Inelastic (3He, t) Scattering from the Ni Isotopes NUCLEAR REACTIONS 58,60,62,64Ni(3He, t), E = 37.5 MeV; measured σ(θ). Coupled-channel analysis, macroscopic, microscopic interaction models.
doi: 10.1103/PhysRev.185.1528
1969RO18 Phys.Letters 30B, 231 (1969) Role of Tensor Force in Charge Exchange Reactions NUCLEAR REACTIONS 54Fe(3He, t), E = 37.7 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(69)90424-9
1966RO01 Phys.Letters 21, 87 (1966) Proton Core Excitation in the Ground State in 18O NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91353-9
1965GL01 Bull.Am.Phys.Soc. 10, No.1, 121, KD3 (1965) C.Glashausser, M.Kondo, M.E.Rickey, E.Rost Evidence for f7/2 Admixture in the Ground State of 40Ca from Neutron Pickup Reactions NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
1965GL02 Phys.Letters 14, 113 (1965) C.Glashausser, M.Kondo, M.E.Rickey, E.Rost Configuration Mixing in the Ground State of Ca40 NUCLEAR STRUCTURE 39Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90443-9
1965SH06 Phys.Rev. 139, B1272 (1965) R.Sherr, B.F.Bayman, E.Rost, M.E.Rickey, C.G.Hoot Excitation of Isobaric Analog States in Medium-Weight Nuclei by the (p, d) Reaction at 28 MeV NUCLEAR STRUCTURE 61Ni, 55Fe, 52Cr, 51Cr, 53Fe, 57Fe, 57Ni, 59Ni, 49Cr, 49Ti, 47Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.139.B1272
1964FU07 Phys.Rev. 134, B117 (1964) H.O.Funsten, N.R.Roberson, E.Rost Inelastic Proton Scattering from Nuclei with 28 Neutrons NUCLEAR STRUCTURE 54Fe, 52Cr, 50Ti, 51V; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.134.117
1964LE10 Phys.Rev. 134, B752 (1964) (p, d) Reactions on Nuclei from V to Ni NUCLEAR STRUCTURE 54Mn, 51Cr, 55Fe, 56Fe, 53Fe, 50V, 59Ni, 57Ni, 58Co, 57Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.134.B752
1964SH12 Phys.Rev.Letters 12, 420 (1964) J Dependence of the Angular Distributions from (p, d) Reaction at 28 Mev NUCLEAR STRUCTURE 59Ni, 57Fe, 57Ni, 55Fe, 61Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.12.420
1962BA67 Phys.Rev. 128, 2693 (1962) R.H.Bassel, G.R.Satchler, R.M.Drisko, E.Rost Analysis of the Inelastic Scattering of Alpha Particles. I
doi: 10.1103/PhysRev.128.2693
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