NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.K.Olsen Found 27 matches. 1994OL02 Nucl.Phys. A570, 243c (1994) The Production of Accelerated Radioactive Ion Beams
doi: 10.1016/0375-9474(94)90289-5
1987OL01 Nucl.Instrum.Methods Phys.Res. A254, 1 (1987) D.K.Olsen, K.A.Erb, C.M.Jones, W.T.Milner, D.C.Weisser, N.F.Ziegler Calibration of the HHIRF Tandem Accelerator Energy-Analyzing Magnet NUCLEAR REACTIONS 12C(16O, α), E=27.3 MeV; measured σ(Eα). Energy analyzing magnet.
doi: 10.1016/0168-9002(87)90474-8
1986AU01 Phys.Rev. C33, 125 (1986) G.F.Auchampaugh, G.de Saussure, D.K.Olsen, R.W.Ingle, R.B.Perez, R.L.Macklin Resolution of the Nature of the Coupling in Subthreshold Fission in 238U + n NUCLEAR REACTIONS 238U(n, γ), (n, n), E=700-740 eV; measured σ(E). 239U deduced resonance, Γn, Γγ, barrier, other parameters.
doi: 10.1103/PhysRevC.33.125
1986OL06 Nucl.Sci.Eng. 94, 102 (1986) Resolved Resonance Parameters for 238U from 1 to 10 keV NUCLEAR REACTIONS 238U(n, X), E=0.9-10 keV; analyzed transmission data. 239U deduced resonances parameters, s-wave strength function. Consistent least squares simultaneous sample shape analysis.
doi: 10.13182/NSE86-A17123
1983OL02 Nucl.Sci.Eng. 83, 174 (1983) Resolved Resonance Parameters for 238U from 4 to 6 keV NUCLEAR REACTIONS 238U(n, X), E=1-100 keV; analyzed transmission data. 239U deduced resonances, (gΓn).
doi: 10.13182/NSE83-A17998
1982OL06 Nucl.Sci.Eng. 82, 289 (1982) D.K.Olsen, R.W.Ingle, J.L.Portney Measurement and Resonance Analysis of the 232Th Total Neutron Cross Section NUCLEAR REACTIONS 232Th(n, X), E=0.007-15 eV, 0.015-4 keV; measured transmission; deduced σ(E). 233Th deduced resonances, parameters, < Γγ >.
doi: 10.13182/NSE82-A19390
1981WI02 Nucl.Sci.Eng. 78, 147 (1981) R.R.Winters, N.W.Hill, R.L.Macklin, J.A.Harvey, D.K.Olsen, G.L.Morgan Uranium-238 Inelastic Neutron Scattering at 82 keV NUCLEAR REACTIONS 238U(n, n'), E=82 keV; measured σ(θ), integrated σ. Legendre polynomial analysis, statistical, optical model calculations.
doi: 10.13182/NSE81-A20100
1980DI05 Phys.Rev. C21, 1400 (1980) F.C.Difilippo, R.B.Perez, G.de Saussure, D.K.Olsen, R.W.Ingle 238U Neutron-Induced Fission Cross Section for Incident Neutron Energies between 5 eV and 3.5 MeV NUCLEAR REACTIONS 238U(n, F), E=5 eV-3.5 MeV; measured σ(E). 239U deduced Γ(F), second well fission barrier parameters.
doi: 10.1103/PhysRevC.21.1400
1980OL06 Nucl.Sci.Eng. 74, 219 (1980) D.K.Olsen, G.L.Morgan, J.W.McConnell Measurement of the 7Li(n, n'γ)7Li' (0.478 MeV) Cross Section from 0.5 to 5.0 MeV NUCLEAR REACTIONS 7Li(n, n'γ), E=0.5-5 MeV; measured Eγ, Iγ, totalσ(Eγ). Ge(Li) detector.
doi: 10.13182/NSE80-A20124
1979OL02 Nucl.Sci.Eng. 69, 202 (1979) D.K.Olsen, G.de Saussure, R.B.Perez, F.C.Difilippo, R.W.Ingle, H.Weaver Measurement and Resonance Analysis of Neutron Transmission Through Uranium-238 NUCLEAR REACTIONS 238U(n, X), E=0.88-100 keV; measured σ. 239U deduced resonance parameters. Multilevel Breit-Wigner fits.
doi: 10.13182/NSE79-A20611
1978DI14 Nucl.Sci.Eng. 68, 43 (1978) F.C.Difilippo, R.B.Perez, G.de Saussure, D.K.Olsen, R.W.Ingle Measurement of the Uranium-238 to Uranium-235 Fission Cross-Section Ratio for Neutron Energies between 0.1 and 25 MeV NUCLEAR REACTIONS 235,238U(n, F), E=0.1-25 MeV; measured ratio of σ.
doi: 10.13182/NSE78-A27269
1978OL01 Nucl.Sci.Eng. 66, 141 (1978) D.K.Olsen, G.de Saussure, R.B.Perez, F.C.Difilippo, R.W.Ingle Note on 238U + n Resolved Resonance Energies NUCLEAR REACTIONS 238U, 32S, 206Pb, 23Na, 27Al(n, n'γ), E=0.1-170 keV; measured transmission spectra. 238U, 32S, 206Pb, 23Na, 27Al deduced neutron resonances.
doi: 10.13182/NSE78-A15200
1977DI13 Nucl.Sci.Eng. 63, 153 (1977) F.C.Difilippo, R.B.Perez, G.de Saussure, D.K.Olsen, R.W.Ingle Measurement of the Uranium-238 Subthreshold Fission Cross Section for Incident Neutron Energies between 0.6 and 100 keV NUCLEAR REACTIONS 238U(n, F), E=0.6-100 keV; measured σ(E). 239U deduced fission barriers.
doi: 10.13182/NSE77-A27019
1977OL03 Nucl.Sci.Eng. 62, 479 (1977) D.K.Olsen, G.de Saussure, R.B.Perez, E.G.Silver, F.C.Difilippo, R.W.Ingle, H.Weaver Precise Measurement and Analysis of Neutron Transmission Through Uranium-238 NUCLEAR REACTIONS 238U(n, n), E=0.52-4000 eV; measured transmission neutron spectra.
doi: 10.13182/NSE77-A26986
1976DE45 Nucl.Sci.Eng. 61, 496 (1976) G.de Saussure, D.K.Olsen, R.B.Perez The ENDF/B-IV Representation of the Uranium-238 Total Neutron Cross Section in the Resolved Resonance Energy Region NUCLEAR REACTIONS 238U(n, X), (n, n'), E ≤ 4 keV; calculated σ(E).
1976FL02 Phys.Rev. C13, 568 (1976) E.R.Flynn, J.D.Sherman, N.Stein, D.K.Olsen, P.J.Riley 84Kr(t, p)86Kr and 86Kr(t, p)88Kr Reactions NUCLEAR REACTIONS 84,86Kr(t, p), E=17.0 MeV; measured σ(Ep, θ). 86,88Kr deduced levels, J, π, L, enhancement.
doi: 10.1103/PhysRevC.13.568
1975CH11 Phys.Rev. C11, 1237 (1975) J.Chao, D.K.Olsen, C.Newsom, P.J.Riley 78,80,82Kr(d, p)79,81,83Kr Reactions NUCLEAR REACTIONS 78,80,82Kr(d, p), E=11 MeV; measured σ(Ep, θ). 80Kr(d, p), E=11 MeV; measured Q. 79,81,83Kr deduced levels, J, π, L, S.
doi: 10.1103/PhysRevC.11.1237
1975OL03 Phys.Rev. C11, 1557 (1975) D.K.Olsen, T.Udagawa, R.E.Brown Study of 20Ne(p, t)18Ne Transitions with the Coupled-Channel Born Approximation NUCLEAR REACTIONS 20Ne(p, t), E=39.8 MeV; measured σ(Et, θ); deduced form factors. 18Ne levels deduced β.
doi: 10.1103/PhysRevC.11.1557
1974AR29 Phys.Rev. C10, 2301 (1974) B.K.Arora, D.K.Olsen, P.J.Riley, C.P.Browne Elastic and Inelastic Scattering of 12.0-MeV Protons from 84,86Kr NUCLEAR REACTIONS 84,86Kr(p, p'), E=12.0 MeV; measured σ(Ep', θ), deduced Q. 84,86Kr deduced levels, J, π, β.
doi: 10.1103/PhysRevC.10.2301
1974BR14 Phys.Rev. C9, 1831 (1974) C.P.Browne, D.K.Olsen, J.Chao, P.J.Riley States in 85Kr from the 84Kr(d, p) Reaction NUCLEAR REACTIONS 84Kr(d, p), E=11 MeV; measured σ(Ep, θ). 85Kr deduced levels, L, S.
doi: 10.1103/PhysRevC.9.1831
1974OL01 Nucl.Phys. A220, 541 (1974) D.K.Olsen, A.R.Barnett, S.F.Biagi, N.H.Merrill, W.R.Phillips Projectile Coulomb Excitation of 20Ne and 22Ne NUCLEAR REACTIONS 197Au, Pt(20Ne, 20Ne'), E=83 MeV; 197Au, Pt(22Ne, 22Ne'), E=91, 80 MeV; measured σ(Eγ, θ). 20,22Ne levels deduced quadrupole moment, B(E2). Projectile Coulomb excitation, reorientation measurement.
doi: 10.1016/0375-9474(74)90134-1
1973HO10 Nucl.Phys. A203, 339 (1973) C.G.Hoot, D.K.Olsen, R.E.Brown, J.R.Maxwell, A.Scott Study of Some Two-Nucleon Pick-up Reactions in the 1p Shell with 39.8 MeV Protons NUCLEAR REACTIONS 12C, 14N, 16O(p, 3He), 14C(p, t), Ep=39.8 MeV; measured σ(E(3He), θ), σ(Et, θ). DWBA analysis.
doi: 10.1016/0375-9474(73)90139-5
1973OL03 Phys.Rev. C8, 609 (1973) D.K.Olsen, T.Udagawa, T.Tamura, R.E.Brown Coupled-Channel-Born-Approximation Analysis of 'Allowed' and 'Forbidden' 22Ne(p, t)20Ne Transitions NUCLEAR REACTIONS 22Ne(p, t), E=39.8 MeV; measured σ(Et, θ). 20Ne deduced nothing.
doi: 10.1103/PhysRevC.8.609
1973UD01 Phys.Lett. 46B, 285 (1973) Note on the 'Forbidden' (p, t) Excitation of Unnatural Parity Final States from 0+ Targets via Multistep Processes NUCLEAR REACTIONS 22Ne(p, t), E=39.8 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(73)90119-6
1972OL02 Phys.Lett. 39B, 201 (1972) D.K.Olsen, W.R.Phillips, A.R.Barnett Static and Dynamic Quadrupole Moments of the First Excited States of 20,22Ne NUCLEAR REACTIONS Au(20Ne, 20Ne'γ), (22Ne, 22Ne'γ), E=4.15 MeV/N; measured Iγ(θ). 20,22Ne levels deduced quadrupole moment, B(E2).
doi: 10.1016/0370-2693(72)90775-7
1972OL04 Phys.Rev.Lett. 29, 1178 (1972); Erratum Phys.Rev.Lett. 30, 940 (1973) D.K.Olsen, T.Udagawa, T.Tamura, R.E.Brown Coupled-Channel Born-Approximation Calculation for the Transition Ne22(p, t)Ne20(2-, 4.97 MeV) NUCLEAR REACTIONS 22Ne(p, t), E=39.8 MeV; measured σ(θ); analyzed σ(θ). Coupled-channel Born approximation; rotational wave functions of adiabatic form.
doi: 10.1103/PhysRevLett.29.1178
1971OL04 Nucl.Phys. A170, 544 (1971) The (p, t) and (p, tau) Reactions on 17O at 39.8 MeV NUCLEAR REACTIONS 17O(p, t), (p, 3He), Ep=39.8 MeV; measured σ(Et, θ), σ(E(3He), θ). Enriched target.
doi: 10.1016/0375-9474(71)90234-X
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