NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.K.Dickens Found 69 matches. 2002BL08 Phys.Rev. C65, 045801 (2002) J.C.Blackmon, S.Raman, J.K.Dickens, R.M.Lindstrom, R.L.Paul, J.E.Lynn Thermal-Neutron Capture by 208Pb NUCLEAR REACTIONS 206,207,208Pb(n, γ), E=subthermal; measured Eγ, Iγ, σ. 209Pb deduced levels, J, π, neutron separation energy. Direct capture model, astrophysical s process.
doi: 10.1103/PhysRevC.65.045801
1996BL10 Phys.Rev. C54, 383 (1996) J.C.Blackmon, A.E.Champagne, J.K.Dickens, J.A.Harvey, M.A.Hofstee, S.Kopecky, D.C.Larson, D.C.Powell, S.Raman, M.S.Smith Measurement of 7Li(n, γ0)8Li Cross Sections at E(n) = 1.5-1340 eV NUCLEAR REACTIONS 7Li(n, γ), E=1.5-1340 eV; measured Eγ, Iγ, γ yield, absolute σ(E); deduced s-wave evidence, normalization relative to 10B(n, αγ) reaction.
doi: 10.1103/PhysRevC.54.383
1993DI02 Nucl.Sci.Eng. 114, 149 (1993) Measurements and Calculations of Radionuclides Created by 181Ta(γ, xnyp) Reactions for Bremsstrahlung Photons Produced by 150-MeV Electrons NUCLEAR REACTIONS, ICPND 181Ta(γ, xnyp), E=150 MeV bremsstrahlung; measured 168mLu to 180Ta yields. Model comparison.
doi: 10.13182/NSE93-A24027
1993SC20 Nucl.Sci.Eng. 114, 352 (1993) R.A.Schrack, O.A.Wasson, D.C.Larson, J.K.Dickens, J.H.Todd A Relative Measurement of the 10B(n, α1γ)7Li Cross Section Between 0.2 and 4.0 MeV NUCLEAR REACTIONS 10B(n, α), E=0.2-4 MeV; measured relative reaction σ. Activation technique.
doi: 10.13182/NSE93-A24044
1989LA10 Phys.Rev. C39, 1736 (1989) 53Cr(n, n'γ) Reactions and the Level Structure of 53Cr NUCLEAR REACTIONS 53Cr(n, n'γ), E=0.6-10 MeV; measured σ(Eγ, E). 53Cr deduced transitions. Enriched sample. Model calculations.
doi: 10.1103/PhysRevC.39.1736
1987DI03 Nucl.Sci.Eng. 96, 8 (1987) Fission Product Yields for Fast-Neutron Fission of 243,244,246,248Cm NUCLEAR REACTIONS 243,244,246,248Cm(n, F)/95Zr/125Sb/137Cs/141Ce/144Ce, 155Er, E=fast; analyzed residual fission product yields, mass distribution data. Mass distribution model.
doi: 10.13182/NSE87-A16359
1986DI02 J.Radioanal.Nucl.Chem. 103, 273 (1986) Half Life of 57Ni RADIOACTIVITY 57Ni(β+), (EC); measured T1/2. Ge(Li) γ-spectrometry.
doi: 10.1007/BF02166003
1986DI09 Phys.Rev. C34, 722 (1986) Yields of Fission Products Produced by Thermal-Neutron Fission of 243Cm NUCLEAR REACTIONS 243Cm(n, F)89Rb/91Sr/91Y/91mY/92Sr/93Sr/94Sr/94Y/95Zr/95Nb/97Zr/97Nb/98Nb/98mNb/99Tc/99mTc/99Mo/101Mo/101Tc/102Tc/102mTc/103Tc/103Ru/104Tc/105Tc/105Ru/105Rh/106Tc/107Ru/107Rh/108Rh/109Rh/112Ag/115In/115mIn/127Sb/128Sn/128Sb/128mSb/129Sb/130Sn/130mSn/130Sb/130mSb/131Sb/131Te/131mTe/131I/132Sb/132mSb/132Te/132I/133I/134I/134mI/135I/135Xe/135mXe/136I/136mI/136Cs/138Xe/139Xe/139Cs/139Ba/140Cs/140Ba/140La/141Ba/142Ba/143Ce/144La/145Ce/146Ce/147Nd/151Pm, E=thermal; measured Eγ, Iγ following fission; deduced residual cumulative yields.
doi: 10.1103/PhysRevC.34.722
1983BE10 Nucl.Sci.Eng. 84, 12 (1983) Z.W.Bell, J.K.Dickens, D.C.Larson, J.H.Todd Neutron-Induced Gamma-Ray Production in 57Fe for Incident Neutron Energies between 0.16 and 21 MeV NUCLEAR REACTIONS 57Fe(n, γ), (n, n'γ), (n, pγ), (n, αγ), E=0.16-21 MeV; measured absolute γ production σ. 57Mn deduced level. 57Fe deduced transitions, transition probability ratios.
doi: 10.13182/NSE83-A17454
1983DI01 Phys.Rev. C27, 253 (1983) Yields of Fission Products Produced by Thermal-Neutron Fission of 229Th NUCLEAR REACTIONS 229Th(n, F), E=thermal; measured γ-yields; deduced cumulative fission yields for 143,141,146Ce, 147,149Nd, 147Pr, 131,133,134,132Te, 85,87,88Kr, 139,141,140,142Ba, 93,91,92Sr, 83Se, 93,91,92,94Y, 131,133,132,134,135I, 140La, 97,95Zr, 130Sb, 84Br, 88Rb.
doi: 10.1103/PhysRevC.27.253
1983DI04 Nucl.Phys. A401, 189 (1983) Gamma-Ray Decay of Levels in 63Cu and 65Cu NUCLEAR REACTIONS 63,65Cu(n, n'γ), E=0.7-6 MeV; measured σ(Eγ, θ=125°). 63,65Cu deduced transitions. Enriched samples.
doi: 10.1016/0375-9474(83)90526-2
1983DI07 Phys.Rev. C28, 916 (1983) Gamma-Ray Transitions among Levels of 206Pb NUCLEAR REACTIONS 206Pb(n, n'γ), E ≤ 8 MeV; measured Eγ, relative Iγ. 206Pb deduced levels, transitions.
doi: 10.1103/PhysRevC.28.916
1983DI10 Phys.Rev. C28, 1404 (1983) Comment on ' Determination of Gamma-Ray Energies and Abudances of 229Th ' RADIOACTIVITY 225Ra [from 229Th(α-decay)]; analyzed Iγ, γ-multipolarity, ICC data; deduced Iγ absolute normalization limits.
doi: 10.1103/PhysRevC.28.1404
1983SL02 Nucl.Sci.Eng. 84, 395 (1983) Gamma-Ray Production due to Neutron Interactions with Copper for Neutron Energies between 0.7 and 10.5 MeV NUCLEAR REACTIONS Cu(n, n'γ), E=0.7-10.5 MeV; measured σ(θγ), total photon yield vs E.
doi: 10.13182/NSE83-A15462
1982DI03 Nucl.Sci.Eng. 80, 455 (1982) J.K.Dickens, J.W.McConnell, K.J.Northcutt Yields of Short-Lived Fission Products of Thermal-Neutron Fission of Thorium-229 NUCLEAR REACTIONS, Fission 229Th(n, F), E=thermal; measured Eγ, Iγ; deduced cumulative yields for 91,90,89Rb, 134,136I, 146,145,148Ce, 139,138,137,140Xe, 148,146Pr, 89,87,90Kr, 142,141Ba, 133,134Te, 130,131,132,133Sb, 84,85,83Se, 144La, 93,94Sr, 140,139Cs, 80As, 88,86Br, 95Y.
doi: 10.13182/NSE82-A19832
1982DI08 Phys.Lett. 113B, 201 (1982) Calculated Beta-Ray Spectra from Decay of Fission Products Produced by Thermal-Neutron Fission of 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; calculated fission fragment decay β-yield vs Eβ.
doi: 10.1016/0370-2693(82)90820-6
1981DI01 Phys.Rev. C23, 331 (1981) Yields of Fission Products Produced by Thermal-Neutron Fission of 245Cm NUCLEAR REACTIONS, Fission 245Cm(n, F), E=thermal; measured σ(Eγ), T1/2. 87,90Kr, 91,93,94Y, 91,92,93,94Sr, 84Br, 88,89Rb, 95,97,99Nb, 99,101Mo, 105,106,103,104,102Tc, 108,109,105,103Ru, 106,111,107,109,105,110Rh, 113,111,114,112Ag, 115In, 131,136,133,137,132,134,135I, 139,137,135,138Xe, 149,147,151Nd, 97,95Zr, 152,153,151Pm, 141,146,148,143,145,136,139,138,140Cs, 139,142,141,140Ba, 132,133,134,131Te, 144,140,142La, 128,127Sn, 146Pr, 127,128,132,129,130,131,133Sb, 156Eu deduced cumulative yields.
doi: 10.1103/PhysRevC.23.331
1981DI02 Nucl.Sci.Eng. 77, 146 (1981) J.K.Dickens, J.W.McConnell, K.J.Northcutt Yields of Short-Lived Fission Products Produced by Thermal-Neutron Fission of Plutonium-239 NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured Eγ, Iγ, T1/2. 90Kr, 106,105,104,101Tc, 108Ru, 146,148,145Ce, 139,138,137Xe, 109Rh, 142,141Ba, 136I, 144La, 133Te, 93,94Sr, 101Mo, 139,140Cs, 132,130Sb, 94Y deduced absolute cumulative yield.
doi: 10.13182/NSE81-A21348
1981DI04 Phys.Rev.Lett. 46, 1061 (1981) Electron Antineutrino Spectrum for 235U(n, f) NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; calculated equilibrium ν-bar yield vs E(ν-bar); deduced average ν-bar energy release, ν-bar induced proton, deuteron disintegration σ. Fission product β-decay input.
doi: 10.1103/PhysRevLett.46.1061
1981DI05 Nucl.Sci.Eng. 78, 126 (1981) J.K.Dickens, T.A.Love, J.W.McConnell, R.W.Peelle Fission-Product Energy Release for Times Following Thermal-Neutron Fission of Plutonium-239 and Plutonium-241 between 2 and 14000 s NUCLEAR REACTIONS, Fission 239,241Pu(n, F), E=thermal; measured β yields, γ-yields, absolute fission-product decay energy release.
doi: 10.13182/NSE81-A20099
1981DI11 Phys.Rev. C24, 192 (1981) Yields of Fission Products Produced by Thermal-Neutron Fission of 249Cf NUCLEAR REACTIONS, Fission 249Cf(n, F), E=thermal; measured Eγ, Iγ, T1/2; deduced partial yields for 103Mo, 103Tc, 109Rh, 109Ru, 112Pd, 112Ag, 119Cd, 119In, 128Sn, 128Sb, 132,134Te, 132,134,135I, 135,138Xe, 138Cs, 146Ce, 146Pr, cumulative yields for 153Sm, 151,149,147Nd, 99,101,104Mo, 105,106,104,103,102Tc, 141,146,148,143,145Ce, 108,107,109,105,103Ru, 139,141,142,140Ba, 139,138,137,135Xe, 134,131,136,133,132,135,134I, 107,105,109,108,106Rh, 130,127,128,132,133Sb, 111,116,114,112Ag, 144,140,142La, 133,134,131Te, 146Pr, 125,128,127Sn, 115,117Cd, 91Y, 93,91,94,92Sr, 140,136,139,138Cs, 97,95Nb, 97,95Zr, 119In, 156Eu, 89Rb.
doi: 10.1103/PhysRevC.24.192
1981DI14 Radiochem.Radioanal.Lett. 47, 331 (1981) Energies and Intensities of Gamma Rays from Decay of 229Th and Daughters in Equilibrium RADIOACTIVITY 229Th, 225Ra, 225Ac, 221Fr, 213Bi, 209Tl; measured Eγ, Iγ following α-decay, β-decay. 225Ra, 225Ac, 221Fr, 217At, 213Bi, 209Tl, 209Bi levels deduced absolute Iγ. 213Po deduced levels, absolute Iγ.
1980DI04 Nucl.Sci.Eng. 73, 42 (1980) Fission Product Yields for Thermal-Neutron Fission of Plutonium-239 NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured Eγ, Iγ, T1/2; deduced cumulative yields for 85,87,88Kr, 88Rb, 91,92Sr, 91,93,94Y, 95,97Zr, 97Nb, 99,101Mo, 103,105,106Ru, 105,107Rh, 104Tc, 127,128,129,130,131Sb, 131,132,133,134Te, 131,133,134,135I, 135,138Xe, 138,139Cs, 139,140Ba, 140,142La, 141,143,144,146Ce, 147Nd, 151Pm.
doi: 10.13182/NSE80-A18707
1980DI13 Phys.Rev. C22, 1344 (1980) Gamma Rays Following Alpha Decay of 245Cm and the Level Structure of 241Pu RADIOACTIVITY 245Cm [from 249Cf(α-decay), chemical separation]; measured Eγ, Iγ, I(K X-ray). 241Pu deduced levels.
doi: 10.1103/PhysRevC.22.1344
1980DI16 Nucl.Instrum.Methods 175, 535 (1980) Absolute Yield of 140.5 keV Gamma Ray Following Decay of 99Mo RADIOACTIVITY 99Mo [from 98Mo(n, γ)]; measured relative Iγ, I(K X-ray); deduced Eβ, Iβ. 99Tc transition deduced absolute Iγ.
doi: 10.1016/0029-554X(80)90769-7
1980DI20 Nucl.Sci.Eng. 74, 106 (1980) J.K.Dickens, T.A.Love, J.W.McConnell, R.W.Peelle Fission-Product Energy Release for Times Following Thermal-Neutron Fission of 235U Between 2 and 14000s NUCLEAR REACTIONS 235U(n, F), E thermal; measured reaction products; deduced fission-product decay energy-release rates based on the separate β- and γ-ray energy-release data.
doi: 10.13182/nse80-a19627
1979DI05 Nucl.Sci.Eng. 70, 177 (1979) Fission Yields for Thermal-Neutron Fission of Plutonium-241 NUCLEAR REACTIONS 241Pu(n, F), E=thermal; measured fission product Eγ. 91Sr, 91,92,93Y, 97Zr, 99Mo, 103,105Rh, 112Ag, 131,133,135I, 132Te, 140Ba, 141,143Ce, 151Pm deduced yields.
doi: 10.13182/NSE79-A19650
1979DI07 Radiochem.Radioanal.Lett. 39, 107 (1979) Half Life of 132Te RADIOACTIVITY 132Te, 99Mo, 131I, 143Ce [from 239Pu(n, F), E=thermal]; measured T1/2.
1977DI11 Nucl.Sci.Eng. 62, 515 (1977) J.K.Dickens, G.L.Morgan, G.T.Chapman, T.A.Love, E.Newman, F.G.Perey Cross Sections for Gamma-Ray Production by Fast Neutrons for 22 Elements between Z = 3 and Z = 82 NUCLEAR REACTIONS Li, C, N, F, Mg, Al, Si, Ca, V, Cr, Fe, Ni, Cu, Zn, Nb, Mo, Ag, Sn, Ta, W, Au, Pb(n, X), E=0.1-20.0 MeV; measured γ production σ.
doi: 10.13182/NSE77-A26989
1977DI12 Nucl.Sci.Eng. 63, 101 (1977) Neutron-Induced Gamma-Ray Production in Lead-208 for Incident-Neutron Energies between 4.9 and 8.0 MeV and in Bismuth-209 for an Incident-Neutron Energy of 5.4 MeV NUCLEAR REACTIONS 208Pb(n, n'γ), E=4.9-8.0 MeV; 209Bi(n, n'γ), E=5.4 MeV; measured γ production σ. 208Pb, 209Bi deduced levels, transitions.
doi: 10.13182/NSE77-A27011
1976MO13 Nucl.Sci.Eng. 60, 36 (1976) Production of Low-Energy Gamma Rays by Neutron Interactions with Fluorine for Incident Neutron Energies between 0.1 and 20 MeV NUCLEAR REACTIONS 19F(n, X), E=0.1-10.2 MeV; measured σ(E, Eγ). 19F, 19O, 16N deduced transitions.
doi: 10.13182/NSE76-A26855
1975DI11 Nucl.Sci.Eng. 58, 331 (1975) Neutron-Induced Gamma-Ray Production in Zinc for Incident-Neutron Energies of 4.9, 5.4, and 5.9 MeV NUCLEAR REACTIONS 64,68Zn, Zn(n, Xγ), E=4.9, 5.4, 5.9 MeV; measured γ-production σ. 64,66,68,67,70Zn deduced transitions.
doi: 10.13182/NSE75-A26783
1974DI07 Nucl.Sci.Eng. 53, 277 (1974) J.K.Dickens, T.A.Love, G.L.Morgan Neutron-Induced Gamma-Ray Production in Calcium in the Energy Range 0.7 < E < 20 MeV NUCLEAR REACTIONS Ca(n, Xγ), E=0.7-20 MeV; measured σ(E, Eγ).
doi: 10.13182/NSE74-A23353
1974DI08 Nucl.Sci.Eng. 54, 191 (1974) Neutron-Induced Gamma-Ray Production in Titanium for Incident-Neutron Energies of 4.9, 5.4, and 5.9 MeV NUCLEAR REACTIONS Ti, 46,48Ti(n, n'γ), E=4.9, 5.4, 5.9 MeV; measured σ(Eγ). 46,47,48,49,50Ti deduced transitions. 46,48Ti deduced levels.
doi: 10.13182/NSE74-A23407
1974DI11 Phys.Rev. C10, 958 (1974) 28Si(n, n'γ) Photon Production Cross Sections for E = 1.78 MeV, 5.0 ≤ E ≤ 9.5 MeV NUCLEAR REACTIONS 28Si(n, n'γ), E=5-9.5 MeV; measured σ(E, Eγ).
doi: 10.1103/PhysRevC.10.958
1973DI06 Nucl.Sci.Eng. 50, 98 (1973) The Neutron-Induced Gamma-Ray Reactions in Sodium-23 in the Energy Range 4.85 < E < 7.5 MeV NUCLEAR REACTIONS 23Na(n, Xγ);E=4.85-7.5; measured Eγ, Iγ; deduced σ(E). 23Na levels deduced γ-branching.
doi: 10.13182/NSE73-A23233
1973DI07 Nucl.Sci.Eng. 50, 311 (1973) J.K.Dickens, G.L.Morgan, F.G.Perey Neutron-Induced Gamma-Ray Production in Iron for the Energy Range 0.8 < E < 20 MeV NUCLEAR REACTIONS 54,56Fe(n, Xγ), E=0.8-20 MeV; measured σ(E, Eγ, θ).
doi: 10.13182/NSE73-A26567
1972DI01 Phys.Rev. C5, 100 (1972) Al(n, xγ) Reactions for 5.3 < E < 9.0 MeV NUCLEAR REACTIONS Al(n, Xγ), E=5.3-9.0 MeV; measured σ(E;Eγ, θ(γ)). 27Al, 27Mg deduced transitions. Ge(Li) detectors.
doi: 10.1103/PhysRevC.5.100
1972DI04 Nucl.Instrum.Methods 98, 451 (1972) Self-Absorption of Gamma Rays Produced in Large Cylindrical Samples
doi: 10.1016/0029-554X(72)90227-3
1972DI07 Phys.Rev. C5, 1977 (1972) Level Structure of 54Mn NUCLEAR REACTIONS 54Fe(n, pγ), E=4.85-6.45 MeV; measured σ(E;Eγ). 54Mn deduced levels, γ-branching, J, π.
doi: 10.1103/PhysRevC.5.1977
1972DI10 Nucl.Sci.Eng. 48, 78 (1972) The Neutron Induced Gamma-Ray Reactions in Calcium in the Energy Range 4.85 < E < 8.05 MeV NUCLEAR REACTIONS 40Ca(n, n'γ), (n, pγ), (n, αγ), E=4.85-8.05 MeV; measured σ(E;Eγ).
doi: 10.13182/NSE72-A22458
1972KU03 Priv.Comm. (January 1972) R.K.Kuebbing, E.Eichler, J.K.Dickens Highly Forbidden E1-Transitions in 92Nb and 94Nb
1972RA21 Phys.Lett. 40B, 89 (1972) S.Raman, N.B.Gove, J.K.Dickens, T.A.Walkiewicz Log ft Values for Second-Forbidden β-Transitions and the Decay of 24Na RADIOACTIVITY 24Na; measured Eγ, Iγ; deduced log ft. 24Mg deduced γ-branching.
doi: 10.1016/0370-2693(72)90291-2
1972ST39 Nucl.Instrum.Methods 98, 481 (1972) P.H.Stelson, J.K.Dickens, S.Raman, R.C.Trammell Deterioration of Large Ge(Li) Diodes Caused by Fast Neutrons
doi: 10.1016/0029-554X(72)90232-7
1970DI10 Phys.Rev. C2, 990 (1970) 28-30si(n, xγ) Reactions for 5.3 < E < 9.0 MeV NUCLEAR REACTIONS 28,29,30Si(n, Xγ), E=5.3-9.0 MeV; measured σ(E;Eγ, θ(γ)). 25Mg, 28Al, 28,29,30Si deduced levels.
doi: 10.1103/PhysRevC.2.990
1970DI18 Nucl.Instrum.Methods 85, 143 (1970) A Monoenergetic 6130-keV Gamma-Ray Source for Detector Calibration NUCLEAR REACTIONS 13C(α, nγ), E=alphas from 244Cm source; measured Eγ.
doi: 10.1016/0029-554X(70)90133-3
1970PE09 Phys.Rev. C2, 468 (1970) C.M.Perey, R.J.Silva, J.K.Dickens, F.G.Perey 11-MeV Proton Inelastic Scattering from Even-Even Medium-Weight Nuclei NUCLEAR REACTIONS 48Ti, 52Cr, 54,56Fe, 60,62,64Ni, 64,66,68Zn, 70,72,74,76Ge(p, p), E=11 MeV; measured nothing; analyzed σ(θ) data. 48Ti, 52Cr, 54,56Fe, 60,62,64Ni, 64,66,68Zn, 70,72,74,76Ge levels deduced β.
doi: 10.1103/PhysRevC.2.468
1968DI05 Phys.Rev. 168, 1355 (1968) J.K.Dickens, E.Eichler, G.R.Satchler 90,92,94Zr(p, p') Reactions at 12.7 MeV NUCLEAR STRUCTURE 94Zr, 92Zr, 90Zr; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.168.1355
1968EI02 Nucl.Phys. A120, 622 (1968) E.Eichler, P.H.Stelson, J.K.Dickens A New Measurement of the Half-Life of the 72Ge 0+ State NUCLEAR REACTIONS 19F, 72Ge(n, n') E=4.75 MeV; measured nX-delay. 19F, 72Ge level deduced T1/2. Natural target.
doi: 10.1016/0375-9474(68)90468-5
1968PE20 Phys.Rev. 175, 1460 (1968) C.M.Perey, F.G.Perey, J.K.Dickens, R.J.Silva 11-MeV Proton Optical-Model Analysis NUCLEAR REACTIONS 48Ti, 51V, 52Cr, 54,56Fe, 59Co, 60,62,64Ni, 63,65Cu, 64,66,68Zn(p, p), E=11 MeV; measured σ(θ); deduced model parameters. Optical model.
doi: 10.1103/PhysRev.175.1460
1968VE06 Phys.Rev. 170, 916 (1968) V.V.Verbinski, F.G.Perey, J.K.Dickens, W.R.Burrus Neutrons from 9Be(α, n) Reaction for E Between 6 and 10 MeV NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.170.916
1967BE23 Phys.Letters 24B, 653 (1967) F.E.Bertrand, J.K.Dickens, T.A.Love Distorted-Wave Analysis of the Inelastic Scattering of 61.7 MeV Protons from 60Ni NUCLEAR STRUCTURE 60Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90370-X
1967CO05 Nucl.Phys. A91, 665(1967) R.K.Cole, R.Dittman, H.S.Sandhu, C.N.Waddell, J.K.Dickens The 19F(p, α)16O and 19F(p, 3He)17O Reactions at 30.5 MeV NUCLEAR REACTIONS 19F(p, α), (p, 3He), E = 30.5 MeV; measured σ(E(He), θ). 16,17O deduced levels, L, S ratios. Natural target.
doi: 10.1016/0375-9474(67)90585-4
1967DI03 ORNL-4182 (1967) J.K.Dickens, F.G.Perey, R.J.Silva Elastic and Inelastic Scattering of 11.0 MeV Protons from 48Ti, 51V, 52Cr, 54Fe, 56Fe, 59Co, 60Ni, 62Ni, 63Cu, 65Cu, 64Zn, 66Zn, and 68Zn: Tabulation of Differential Cross-Sections NUCLEAR STRUCTURE 68Zn, 63Cu, 66Zn, 64Zn, 64Ni, 62Ni, 65Cu, 48Ti, 60Ni, 59Co, 52Cr, 52V, 54Fe, 56Fe; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2165. 1967DI05 Nucl.Phys. A101, 408(1967) The 91Zr(d, p)92Zr Reaction at E = 6.25 MeV NUCLEAR REACTIONS 91Zr(d, p), E=6.25 MeV; measured σ(Ep, θ). 92Zr deduced levels, L. Enriched target.
doi: 10.1016/0375-9474(67)90195-9
1967ST19 Priv.Comm. (1967) P.H.Stelson, J.K.Dickens, F.G.Perey NUCLEAR STRUCTURE 59Ni; measured not abstracted; deduced nuclear properties.
1966DI01 Phys.Lett. 21, 657 (1966) J.K.Dickens, E.Eichler, R.J.Silva, I.R.Williams Level Structure of 92Mo NUCLEAR STRUCTURE 92Mo; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90114-4
1965DI02 Phys.Rev. 138, B1083 (1965) Elastic Scattering of Low-Energy Deuterons from 60Ni and 114Cd and the Effect of the Deuteron Electric Polarizability in the Optical-Model Potential NUCLEAR STRUCTURE 114Cd, 60Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.138.B1083
1965DI09 Nucl.Phys. 73, 529 (1965) J.K.Dickens, F.G.Perey, G.R.Satchler Inelastic Scattering of Deuterons from 60Ni and 114Cd NUCLEAR REACTIONS 60Ni(d, d'), E = 9.89, 10.86, 11.92, 13.56 MeV; 114Cd(d, d'), E = 8, 9, 10, 11, 12, 13, 14, 15 MeV; measured σ(Ed', θ). 60Ni, 114Cd deduced deformation. Enriched targets.
doi: 10.1016/0029-5582(65)90698-X
1965DI11 ORNL-3851 (1965) Elastic and Inelastic Scattering of 12.0-MeV Protons from 62Ni, 63Cu, and 64Zn: Tabulated Differential Cross Sections NUCLEAR STRUCTURE 63Cu, 64Zn, 62Ni; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2175. 1965DI12 ORNL-3858, Vol.1, p.3 (1965) J.K.Dickens, F.G.Perey, R.J.Silva Level Structure of 64Zn NUCLEAR STRUCTURE 64Zn; measured not abstracted; deduced nuclear properties.
1963DI04 Phys.Rev. 129, 743 (1963) J.K.Dickens, D.A.Haner, C.N.Waddell Elastic and Inelastic Scattering of 31.1-MeV Protons by Carbon-12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.743
1963DI11 Phys.Lett. 6, 53 (1963) J.K.Dickens, F.G.Perey, R.J.Silva, T.Tamura Proton Excitation of Two-Phonon Levels NUCLEAR STRUCTURE 64Ni, 62Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90219-1
1963DI14 Conf.Compd. Nucl.States, Gatlinburg, Tenn. p.38, CB6 (1963) J.K.Dickens, F.G.Perey, R.J.Silva Fluctuations in the Excitation Function for Elastic and Inelastic Scattering of Protons from Ni62 NUCLEAR STRUCTURE 62Ni; measured not abstracted; deduced nuclear properties.
1963DI15 Phys.Rev. 132, 1190 (1963) J.K.Dickens, F.G.Perey, R.J.Silva Level Structure of Ni64 NUCLEAR STRUCTURE 64Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.132.1190
1963DI16 Phys.Rev. 132, 2159 (1963) J.K.Dickens, D.A.Haner, C.N.Waddell Elastic and Inelastic Scattering of Protons by Carbon-12 for Proton Energies between 18 and 30 MeV NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.132.2159
1963DI18 WASH-1044, p.66 (1963) J.K.Dickens, F.G.Perey, R.J.Silva Inelastic Scattering of 11 MeV Protons from Medium Weight Nuclei NUCLEAR STRUCTURE 70Ge, 76Ge, 72Ge, 74Ge; measured not abstracted; deduced nuclear properties.
1962DI02 Bull.Am.Phys.Soc. 7, No.4, 285, FB4 (1962) J.K.Dickens, D.A.Haner, C.N.Waddell Differential Elastic Scattering of Protons from C12 for Proton Energies between 20 and 31 MeV NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1962WA06 Bull.Am.Phys.Soc. 7, No.4, 285, FB3 (1962) C.N.Waddell, J.K.Dickens, D.A.Haner Differential Elastic and Inelastic Scattering of 31.1-MeV Protons from C12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
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