NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.K.Bockelman Found 55 matches. 1980MO11 Phys.Rev. C21, 2275 (1980) M.H.Mortensen, R.R.Betts, C.K.Bockelman W(p, t) Reactions. I. Even Targets NUCLEAR REACTIONS 186,184,182,180W(p, t), E=21 MeV; measured σ(Et, θ). 180W(t, p), E=15 MeV; measured σ(Ep, θ). 184,182,180,178W deduced levels, L, π, J, band structure. DWBA, CCBA analyses.
doi: 10.1103/PhysRevC.21.2275
1980MO12 Phys.Rev. C21, 2288 (1980) M.H.Mortensen, R.R.Betts, C.K.Bockelman W(p, t) Reactions. II. Odd Target NUCLEAR REACTIONS 183W(p, t), E=21 MeV; measured σ(Et, θ). 181W deduced levels, L, π, J, band structure, configuration. DWBA analysis.
doi: 10.1103/PhysRevC.21.2288
1977MA03 Phys.Rev. C15, 161 (1977) C.F.Maguire, W.D.Callender, D.G.Kovar, C.K.Bockelman States in 205Pb Excited via the 204Pb(d, p) Reaction. I. The 'Hole' States NUCLEAR REACTIONS 204Pb(d, p), E=13.0, 20.0 MeV; measured σ(Ep, θ). 205Pb levels deduced S.
doi: 10.1103/PhysRevC.15.161
1977MA04 Phys.Rev. C15, 170 (1977) C.F.Maguire, D.G.Kovar, W.D.Callender, C.K.Bockelman States in 205Pb Excited via the 204Pb(d, p) Reaction. II. The 'Particle' States NUCLEAR REACTIONS 204Pb(d, p), E=13.0, 20.0 MeV; 208Pb(d, p), E=13.0 MeV; measured σ(Ep, θ). 205Pb deduced levels, S. 208Pb(d, p), E=18.7, 20, 24.8 MeV; 206Pb(d, p), E=17.0 MeV; analyzed previous data. Weak coupling theory.
doi: 10.1103/PhysRevC.15.170
1977MO15 Phys.Lett. 70B, 17 (1977) M.H.Mortensen, R.R.Betts, C.K.Bockelman Pair Excitations in the Even W-Isotopes NUCLEAR REACTIONS W(p, t), E=21 MeV; measured σ(Et, θ). 178,180,182W deduced levels, J, π.
doi: 10.1016/0370-2693(77)90333-1
1975ME15 Phys.Rev. C12, 827 (1975) W.D.Metz, W.D.Callender, C.K.Bockelman Forbidden Transitions in the 48Ca(d, p)49Ca Reaction NUCLEAR REACTIONS 48Ca(d, p), E=9, 13, 16, 19.3, 20 MeV; measured σ(Ep, θ). 48Ca(d, d), E=9, 13, 16, 19.3, 20 MeV; measured σ(θ). 49Ca deduced levels, J, π, S, L.
doi: 10.1103/PhysRevC.12.827
1974KO20 Nucl.Phys. A231, 266 (1974) D.G.Kovar, N.Stein, C.K.Bockelman Excitation of Two-Particle-One-Hole States by the 208Pb(d, p)209Pb Reaction NUCLEAR REACTIONS 208Pb(d, p), E=20 MeV; measured σ(Ep, θ); deduced Q. 209Pb deduced levels, J, π, S, L. Enriched targets.
doi: 10.1016/0375-9474(74)90522-3
1974YE01 Nucl.Phys. A235, 135 (1974) R.Yen, L.S.Cardman, D.Kalinsky, J.R.Legg, C.K.Bockelman Determination of Nuclear Parameters by Inelastic Electron Scattering at Low-Momentum Transfer NUCLEAR REACTIONS 6Li, 60Ni, 114Cd(e, e'), E=30-60 MeV; measured σ(E, Ee', θ). 6Li, 60Ni, 114Cd levels deduced form factors, B(E2), transition radii.
doi: 10.1016/0375-9474(74)90182-1
1973CA33 Nucl.Phys. A216, 285 (1973) L.S.Cardman, D.Kalinsky, J.R.Legg, R.Yen, C.K.Bockelman Search for Dispersive Effects in Electron Scattering from Samarium NUCLEAR REACTIONS 148,150,152Sm(e, e), E=42, 60 MeV; measured σ(E, θ). Deduced charge distribution parameters. Enriched targets. 142,146,150Nd(e, e); reanalyzed data.
doi: 10.1016/0375-9474(73)90469-7
1973KA44 Nucl.Phys. A216, 312 (1973) D.Kalinsky, L.S.Cardman, R.Yen, J.R.Legg, C.K.Bockelman Electron Scattering Studies of 184W and 186W NUCLEAR REACTIONS 184,186W(e, e), E=42, 60, 65 MeV; measured σ(E, θ). Deduced charge distribution parameters. Enriched targets.
doi: 10.1016/0375-9474(73)90470-3
1971MA27 Nucl.Phys. A168, 97 (1971) D.W.Madsen, L.S.Cardman, J.R.Legg, C.K.Bockelman Anomalous Electron Scattering from 142,146,150Nd NUCLEAR REACTIONS 142,146,150Nd(e, e), (e, e'), E=40, 60 MeV; measured σ(θ). 142,146,150Nd levels deduced J, π, B(EL ).
doi: 10.1016/0375-9474(71)90653-1
1969CU06 Phys.Rev. 184, 1162 (1969) T.H.Curtis, R.A.Eisenstein, D.W.Madsen, C.K.Bockelman Quadrupole and Octupole Excitations of the Even Tin Isotopes by Electron Scattering NUCLEAR REACTIONS 116,118,120Sn(e, e') , E = 60 MeV; measured σ(Ee'); deduced elastic, inelastic form factors. 116,118,120Sn deduced B(EL).
doi: 10.1103/PhysRev.184.1162
1969EI03 Phys.Rev. 188, 1815 (1969) R.A.Eisenstein, D.W.Madsen, H.Theissen, L.S.Cardman, C.K.Bockelman Electron-Scattering Studies on Ca40 and Ca48 NUCLEAR REACTIONS 40,48Ca(e, e), (e, e'), E=20-60 MeV; measured σ(E;Ee', θ); deduced elastic, inelastic form factors. 40,48Ca deduced nuclear radii, B(EL).
doi: 10.1103/PhysRev.188.1815
1969MA29 Phys.Rev.Letters 23, 1122 (1969) D.W.Madsen, L.S.Cardman, J.R.Legg, E.F.Gundersheim, C.K.Bockelman Anomalous Electron Scattering from Nd142 NUCLEAR REACTIONS 142Nd(e, e), E = 15-60 MeV; measured σ(E;θ). 142Nd deduced nuclear charge distribution.
doi: 10.1103/PhysRevLett.23.1122
1968WI02 Phys.Rev. 166, 1121 (1968) P.Wilhjelm, O.Hansen, J.R.Comfort, C.K.Bockelman, P.D.Barnes, A.Sperduto Inelastic Deuteron Scattering and (d, p) Reactions from Isotopes of Ti. V. Ti(d, d') NUCLEAR STRUCTURE 48Ti, 47Ti, 50Ti, 49Ti, 51Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.166.1121
1967BA15 Phys.Rev. 155, 1319 (1967) P.D.Barnes, J.R.Comfort, C.K.Bockelman Vibrational Spectrum of Cd112 NUCLEAR STRUCTURE 112Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.155.1319
1967BA32 Phys.Rev.159, 920 (1967) P.D.Barnes, J.R.Comfort, C.K.Bockelman, O.Hansen, A.Sperduto Inelastic Deuteron Scattering and (d, p) Reactions from Isotopes of Titanium. IV. Ti48(d, p)Ti49 NUCLEAR REACTIONS 48Ti(d, p), E=6 MeV; measured σ(Ep, θ); deduced Q. 49Ti deduced levels, L(n), S, J, π.
doi: 10.1103/PhysRev.159.920
1967CO15 Phys.Rev. 157, 1065 (1967) J.R.Comfort, C.K.Bockelman, P.D.Barnes Vibrational Spectrum in Cd114 NUCLEAR STRUCTURE 114Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.157.1065
1967DU07 Phys.Rev. 163, 1259 (1967) M.A.Duguay, C.K.Bockelman, T.H.Curtis, R.A.Eisenstein Inelastic Electron Scattering from Ni58, Ni60, and Ni62 NUCLEAR REACTIONS 58,60,62Ni(e, e'), E=40-70 MeV; measured σ(E;Ee'); deduced form factors. 58,60,62Ni levels deduced B(EL), transition radii.
doi: 10.1103/PhysRev.163.1259
1967WE02 Nucl.Phys. A92, 696 (1967) K.J.Wetzel, C.K.Bockelman, O.A.Wasson Gamma Rays from Thermal and Resonance Neutron Capture in Gold NUCLEAR REACTIONS 197Au(n, γ), E = thermal, 4.9 eV; measured Eγ, Iγ. 198Au deduced levels. Ge(Li) detector.
doi: 10.1016/0375-9474(67)90639-2
1966CU03 Bull.Am.Phys.Soc, 11, No.3, 351, EB3 (1966) T.H.Curtis, M.A.Duguay, R.A.Eisenstein, C.K.Bockelman Inelastic Electron Scattering from the Nuclei Ni58, Ni60, Ni62 NUCLEAR STRUCTURE 60Ni, 58Ni, 62Ni; measured not abstracted; deduced nuclear properties.
1966DU02 Phys.Rev.Letters 17, 28 (1966) M.A.Duguay, C.K.Bockelman, T.H.Curtis, R.A.Eisenstein Inelastic Electron Scattering from the First Excited State of 58Ni, 60Ni, and 62Ni NUCLEAR STRUCTURE 58Ni, 60Ni, 62Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.17.28
1965BA01 Bull.Am.Phys.Soc. 10, No.1, 39, CD6 (1965) P.D.Barnes, C.K.Bockelman, O.Hansen, A.Sperduto Ti50 Levels Excited by the Ti49(d, p) Reaction NUCLEAR STRUCTURE 50Ti; measured not abstracted; deduced nuclear properties.
1965BA07 Phys.Rev. 138, B597 (1965) P.D.Barnes, C.K.Bockelman, O.Hansen, A.Sperduto Inelastic Deuteron Scattering and (d, p) Reactions from Isotopes of Ti. II. Ti47(d, p)Ti48 NUCLEAR STRUCTURE 48Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.138.B597
1965BA22 Phys.Rev. 140, B42 (1965) P.D.Barnes, C.K.Bockelman, O.Hansen, A.Sperduto Inelastic Deuteron Scattering and (d, p) Reactions from Isotopes of Titanium. III. Ti49(d, p)Ti50 NUCLEAR STRUCTURE 50Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B42
1965WE01 Bull.Am.Phys.Soc. 10, No.1, 13, AD10 (1965) K.J.Wetzel, O.A.Wasson, C.K.Bockelman γ-Rays from Neutron Capture in Gold NUCLEAR STRUCTURE 198Au; measured not abstracted; deduced nuclear properties.
1964BA39 Phys. Rev. 136, B438 (1964) P.D.Barnes, C.K.Bockelman, O.Hansen, A.Sperduto Inelastic Deuteron Scattering and (d, p) Reactions from Isotopes of Ti. I. Ti50(d, p)Ti51 NUCLEAR STRUCTURE 51Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.136.B438
1964WA16 Phys.Rev. 136, B1640 (1964) O.A.Wasson, K.J.Wetzel, C.K.Bockelman Gamma Rays from Thermal Neutron Capture in Cl, V, Mn, and Co NUCLEAR STRUCTURE 35Cl, 51V, 52V, 55Mn, 60Co, 59Co, Mn, Co, Cl, V; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.136.B1640
1963BA14 Bull.Am.Phys.Soc. 8, No.4, 367, R7 (1963) P.D.Barnes, C.K.Bockelman, O.Hansen, A.Sperduto, W.W.Buechner Ti50(d, p)Ti51 Reactions NUCLEAR STRUCTURE 51Ti; measured not abstracted; deduced nuclear properties.
1959FE16 Nuclear Phys. 10, 386 (1959) C.A.Fenstermacher, J.E.Draper, C.K.Bockelman Resonant Neutron Capture in Er and Hf
doi: 10.1016/0029-5582(59)90227-5
1958DR71 Bull.Am.Phys.Soc. 3, No.3, 177, F8 (1958) Low-Energy Gamma Rays from Thermal Neutron Capture
1957BO08 Bull.Am.Phys.Soc. 2, No.1, 41, NA2 (1957); Oral Report C.K.Bockelman, C.A.Fenstermacher, J.E.Draper Rotational Levels in Hf178 Excited by Resonance Neutron Capture
1957BO99 Phys.Rev. 107, 176 (1957) C.K.Bockelman, C.M.Braams, C.P.Browne, W.W.Buechner, R.R.Sharp, A.Sperduto Angular Distribution of Protons from the Ca42(d, p)Ca43 Reaction
doi: 10.1103/PhysRev.107.176
1957BP01 Phys.Rev. 107, 1366 (1957) Angular Distribution of Protons from the Ca40(d, p)Ca41 Reaction
doi: 10.1103/PhysRev.107.1366
1957BR12 Phys.Rev. 105, 1301 (1957) Comparison of Energy Levels of Li6 from Various Reactions
doi: 10.1103/PhysRev.105.1301
1957EL11 Phys.Rev. 105, 657 (1957) Inelastic Proton Scattering from Gold at 6 MeV
doi: 10.1103/PhysRev.105.657
1957FE31 Phys.Rev. 107, 1650 (1957) C.A.Fenstermacher, R.G.Bennett, A.E.Walters, C.K.Bockelman, H.L.Schultz Absolute Intensities of Resonance Capture Gamma Rays from Cd, Te, and Sm
doi: 10.1103/PhysRev.107.1650
1957SC31 Proc.Intern.Conf.Neutron Interactions with the Nucleus, New York, p.266 (1957); TID-7547 (1957) H.L.Schultz, C.K.Bockelman, J.Draper, C.A.Fenstermacher, L.Rosler Gamma Rays Following Resonant Neutron Capture
1956BO18 Phys.Rev. 104, 456 (1956) C.K.Bockelman, A.Leveque, W.W.Buechner Energy Levels of Be9
doi: 10.1103/PhysRev.104.456
1954JU23 Phys.Rev. 96, 1353 (1954) Energy Levels of Be10*
doi: 10.1103/PhysRev.96.1353
1954SP01 Phys.Rev. 96, 1316 (1954) A.Sperduto, W.W.Buechner, C.K.Bockelman, C.P.Browne (d, p) Reactions from Carbon, Nitrogen, and Oxygen
doi: 10.1103/PhysRev.96.1316
1953BO70 Phys.Rev. 92, 665 (1953) C.K.Bockelman, C.P.Browne, W.W.Buechner, A.Sperduto Inelastic Scattering of Protons and Deuterons from B10 and N14
doi: 10.1103/PhysRev.92.665
1953BU98 Phys.Rev. 91, 1502 (1953) W.W.Buechner, A.Sperduto, C.P.Browne, C.K.Bockelman Excited States of K40 NUCLEAR REACTIONS 39K(d, p), E=4.76, 5.00, 5.16, 5.65 MeV; measured Ep. 40K deduced excited states energies.
doi: 10.1103/PhysRev.91.1502
1952BU81 Phys.Rev. 87, 237 YA2 (1952) W.W.Buechner, C.P.Browne, M.M.Elkind, A.Sperduto, H.A.Enge, C.K.Bockelman Inelastic Proton Scattering from B10 NUCLEAR REACTIONS 10B(p, p'), E=7 MeV; measured reaction products, Ep, Ip; deduced energy levels. Comparison with available data.
doi: 10.1103/PhysRev.87.179
1952MI56 Phys.Rev. 88, 83 (1952) D.W.Miller, R.K.Adair, C.K.Bockelman, S.E.Darden Total Cross Sections Of Heavy Nuclei For Fast Neutrons NUCLEAR REACTIONS Fe(n, x), Ni(n, x), Cu(n, x), Zn(n, x), Sr(n, x), 89Y(n, x), Zr(n, x), 93Nb(n, x), Mo(n, x), Ag(n, x), In(n, x), Sn(n, x), Sb(n, x), 127I(n, x), Ba(n, x), La(n, x), Ce(n, x), 141Pr(n, x), Ta(n, x), W(n, x), Pb(n, x), 206Pb(n, x), 209Bi(n, x), E=5 keV-3.2 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 11712.
doi: 10.1103/PhysRev.88.83
1951BO45 Phys.Rev. 84, 69 (1951) C.K.Bockelman, D.W.Miller, R.K.Adair, H.H.Barschall Total Cross Sections of Light Nuclei for p, T-Neutrons
doi: 10.1103/PhysRev.84.69
1951CO51 Phys.Rev. 81, 33 (1951) J.H.Coon, C.K.Bockelman, H.H.Barschall Angular Distribution Of 14-Mev Neutrons Scattered By Tritons NUCLEAR REACTIONS 3H(n, n), E=14.3 MeV; measured products, 3H; deduced σ(θ). Data were imported from EXFOR entry 11040.
doi: 10.1103/PhysRev.81.33
1951JO22 Phys.Rev. 82, 117 (1951) C.H.Johnson, C.K.Bockelman, H.H.Barschall Disintegration Of Neon By Fast Neutrons NUCLEAR REACTIONS 20Ne(n, α), E=1.8-3.3 MeV; measured products, 17O, 4He; deduced σ, σ(E). Data were imported from EXFOR entry 11385.
doi: 10.1103/PhysRev.82.117
1950BA88 Phys.Rev. 79, 593 (1950) R.E.Peterson, H.H.Barschall, C.K.Bockelman Investigation of Nuclear Energy Levels in Sulfur NUCLEAR REACTIONS S(n, γ), E=15-1450 keV; measured En, In, and total neutron σ. 32S; deduced neutron resonances. 33S; deduced levels.
doi: 10.1103/PhysRev.79.593
1950BO95 Phys.Rev. 80, 1011 (1950) Total Cross Sections Of Be, B, O And F For Fast Neutrons NUCLEAR REACTIONS 9Be(n, x), B(n, x), O(n, x), , 19F(n, x), E=10 keV-1.4 MeV; measured products; deduced σ, σ(E), resonance parameters. Data were imported from EXFOR entry 11208.
doi: 10.1103/PhysRev.80.1011
1949AD01 Phys.Rev. 75, 1124 (1949) R.K.Adair, H.H.Barschall, C.K.Bockelman, O.Sala Total Cross Section of Be, O, Na, and Ca for Fast Neutrons NUCLEAR REACTIONS Be, O, Na, Ca(n, X), E=30-1000 keV; measured total σ; deduced resonances.
doi: 10.1103/PhysRev.75.1124
1949AD02 Phys.Rev. 76, 308 (1949) R.K.Adair, C.K.Bockelman, R.E.Peterson Experimental Corroboration Of The Theory Of Neutron Resonance ScatterIng NUCLEAR REACTIONS S, 32S(n, x), E=-1.0 eV-205 keV; measured products; deduced σ, σ(E), resonance parameters. Data were imported from EXFOR entry 11582.
doi: 10.1103/PhysRev.76.308
1949BA42 Phys.Rev. 76, 1146 (1949) H.H.Barschall, C.K.Bockelman, R.E.Peterson, R.K.Adair Investigation Of Nuclear Energy Levels In Lead NUCLEAR REACTIONS Pb(n, x), 209Bi(n, x), E=18-761 keV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 12228.
doi: 10.1103/PhysRev.76.1146
1949BO68 Phys.Rev. 76, 277 (1949) C.K.Bockelman, R.E.Peterson, R.K.Adair, H.H.Barschall Total Cross Section Measurements For Fast Neutrons NUCLEAR REACTIONS Zr(n, x), Ag(n, x), In(n, x), Sb(n, x), 127I(n, x), Ta(n, x), Pb(n, x), E=12 keV-1.5 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 11881.
doi: 10.1103/PhysRev.76.277
1948BA01 Phys.Rev. 73, 659 (1948) H.H.Barschall, C.K.Bockelman, L.W.Seagondollar Total Cross Section of Fe, Ni, and Bi for Fast Neutrons NUCLEAR REACTIONS 209Bi, Fe, Ni(n, X), E<1.4 MeV; measured reaction products, En, In; deduced σ, thick target yields. Comparison with available data.
doi: 10.1103/PhysRev.73.659
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