NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = L.F.Hansen Found 44 matches. 1995SA04 Phys.Rev. C51, 1280 (1995) T.C.Sangster, M.Begemann-Blaich, Th.Blaich, H.C.Britt, L.F.Hansen, M.N.Namboodiri, G.Peilert Correlations of Intermediate Mass Fragments from Fe + Ta, Au, and Th Collisions NUCLEAR REACTIONS 182Ta, 197Au, 232Th(Fe, X), E=50-100 MeV/nucleon; measured σ(θ) vs fragment Z, velocity; deduced fragmenting source extent. Quantum molecular dynamics approach.
doi: 10.1103/PhysRevC.51.1280
1994HJ01 Phys.Rev. C50, 275 (1994) E.L.Hjort, F.P.Brady, J.L.Romero, J.R.Drummond, D.S.Sorenson, J.H.Osborne, B.McEachern, L.F.Hansen Measurements and Analysis of Neutron Elastic Scattering at 65 MeV NUCLEAR REACTIONS C, Si, Cd, Fe, Sn, Pb(n, n), E=65 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1103/PhysRevC.50.275
1993PE13 Nucl.Phys. A563, 387 (1993) F.Petrovich, S.K.Yoon, M.J.Threapleton, R.J.Philpott, J.A.Carr, F.S.Dietrich, L.F.Hansen Consistent Folding Model Description of Nucleon Elastic, Inelastic, and Charge-Exchange Scattering from 6,7Li at 25-50 MeV NUCLEAR REACTIONS 6Li(p, p), E=24.4-49.75 MeV; analyzed σ(θ). 7Li(polarized p, p), (polarized p, p'), E=24.4, 49.75, 200 MeV; analyzed σ(θ), analyzing power vs θ. Folding model.
doi: 10.1016/0375-9474(93)90120-M
1992BE01 Phys.Rev. C45, 677 (1992) M.Begemann-Blaich, Th.Blaich, M.M.Fowler, J.B.Wilhelmy, H.C.Britt, D.J.Fields, L.F.Hansen, R.G.Lanier, D.J.Massoletti, M.N.Namboodiri, B.A.Remington, T.C.Sangster, G.L.Struble, M.L.Webb, Y.D.Chan, A.Dacal, A.Harmon, J.Pouliot, R.G.Stokstad, S.Kaufman, F.Videbaek, Z.Fraenkel Fission from Fe and Nb Reactions with Heavy Targets at 50-100 MeV/Nucleon NUCLEAR REACTIONS Ta, 197Au, Th(Fe, F), (93Nb, F), E=50-100 MeV/nucleon; measured fission σ, charge loss distribution, fragment velocity systematics, momentum transfers. Peripheral collisions, model analysis.
doi: 10.1103/PhysRevC.45.677
1992BL01 Phys.Rev. C45, 689 (1992) Th.Blaich, M.Begemann-Blaich, M.M.Fowler, J.B.Wilhelmy, H.C.Britt, D.J.Fields, L.F.Hansen, M.N.Namboodiri, T.C.Sangster, Z.Fraenkel Calculation for Fission Decay from Heavy Ion Reactions at Intermediate Energies NUCLEAR REACTIONS Ta, 197Au, Th(Fe, F), (93Nb, F), E=100 MeV/nucleon; analyzed data. Intranuclear cascade model, final state statistical evaporation decay.
doi: 10.1103/PhysRevC.45.689
1992SA15 Phys.Rev. C46, 1404 (1992) T.C.Sangster, H.C.Britt, D.J.Fields, L.F.Hansen, R.G.Lanier, M.N.Namboodiri, B.A.Remington, M.L.Webb, M.Begemann-Blaich, T.Blaich, M.M.Fowler, J.B.Wilhelmy, Y.D.Chan, A.Dacal, A.Harmon, J.Pouliot, R.G.Stokstad, S.Kaufman, F.Videbaek, Z.Fraenkel, G.Peilert, H.Stocker, W.Greiner, A.Botvina, I.N.Mishustin Intermediate Mass Fragment Emission in Fe + Au Collisions NUCLEAR REACTIONS 197Au(Fe, X), E=50-100 MeV/nucleon; measured σ(fragment θ), charge, velocity distributions; deduced intermediate mass fragment production mechanism. Quantum molecular dynamics model.
doi: 10.1103/PhysRevC.46.1404
1989FI07 Nucl.Phys. A495, 209c (1989) D.J.Fields, T.C.Sangster, M.L.Webb, B.A.Remington, H.C.Britt, L.F.Hansen, R.G.Lanier, D.Massoletti, M.N.Namboodiri, G.L.Struble, M.L.Begemann-Blaich, T.Blaich, M.M.Fowler, J.Wilhelmy, S.Kaufman, F.Videbaek, Y.D.Chan, A.Dacal, A.Harmon, J.Pouliot, R.Stokstad, Z.Fraenkel Heavy Ion Reaction Studies of Nb + Au at E/A = 50, 75 and 100 MeV NUCLEAR REACTIONS 197Au(93Nb, F), E=50-100 MeV/nucleon; measured fission (fragment)(fragment)-coin, (fragment)(fragment)(θ); deduced fission mechanism.
doi: 10.1016/0375-9474(89)90320-5
1989MA44 Phys.Rev. C40, 1999 (1989) V.A.Madsen, L.F.Hansen, V.R.Brown, D.G.Madland Correction for Truncation in Coupled-Channels Optical Potentials NUCLEAR REACTIONS 238U(n, n'), E=1, 4, 8 MeV; 238U(p, p'), E=18, 26 MeV; calculated σ. Coupled-channels formalism, truncation.
doi: 10.1103/PhysRevC.40.1999
1988HA25 Phys.Rev. C38, 525 (1988) L.F.Hansen, J.Rapaport, X.Wang, F.A.Barrios, F.Petrovich, A.W.Carpenter, M.J.Threapleton Proton and Neutron Transition Densities in 6,7Li from Low Energy Neutron and Proton Scattering NUCLEAR REACTIONS 6,7Li(n, n), (n, n'), E=24 MeV; measured σ(θ). 6,7Li deduced transition densities.
doi: 10.1103/PhysRevC.38.525
1986HA31 Radiat.Eff. 92, 83 (1986) Measurements and Calculations of Neutron Scattering Angular Distributions Over a Wide Mass and Energy Range NUCLEAR REACTIONS 9Be, C, 27Al, Fe, 59Co, 89Y, 93Nb, In, 140Ce, 181Ta, 197Au, 208Pb, 209Bi, 232Th, 238U, 239Pu(n, n), E=14.6 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1080/00337578608208298
1986HA44 Phys.Rev. C34, 2075 (1986) L.F.Hansen, B.A.Pohl, C.Wong, R.C.Haight, Ch.Lagrange Measurements and Calculations of Neutron Scattering in the Actinide Region NUCLEAR REACTIONS 232Th, 238U, 239Pu(n, n), E=14.1 MeV; measured σ(E, θ=0°); deduced semi-microscopic, deformed optical model potentials.
doi: 10.1103/PhysRevC.34.2075
1985BL12 Phys.Rev. C32, 411 (1985) M.Blann, S.M.Grimes, L.F.Hansen, T.T.Komoto, B.A.Pohl, W.Scobel, M.Trabandt, C.Wong Single-Particle Effects in Precompound Reactions: Influence of the f7/2 shell closure NUCLEAR REACTIONS 50,52,53Cr, 58Fe, 59Co, 60Ni, 63Cu(p, n), E=25 MeV; measured angle integrated neutron spectra; deduced precompound emission shell dependence.
doi: 10.1103/PhysRevC.32.411
1985HA02 Phys.Rev. C31, 111 (1985) L.F.Hansen, F.S.Dietrich, B.A.Pohl, C.H.Poppe, C.Wong Test of Microscopic Optical Model Potentials for Neutron Elastic Scattering at 14.6 MeV over a Wide Mass Range NUCLEAR REACTIONS 9Be, C, 27Al, Fe, 59Co, 93Nb, 89Y, In, 140Ce, 181Ta, 197Au, 208Pb, 209Bi(n, n), E=14.6 MeV; measured σ(θ). Local microscopic potentials, optical model analysis.
doi: 10.1103/PhysRevC.31.111
1984SC33 Phys.Rev. C30, 1480 (1984) W.Scobel, M.Blann, T.T.Komoto, M.Trabandt, S.M.Grimes, L.F.Hansen, C.Wong, B.A.Pohl Single Particle Effects in Precompound Reactions NUCLEAR REACTIONS 50,52,53Cr, 54,56,58Fe, 59Co, 60Ni, 63Cu, 89Y, 90,91,92,94Zr, 92,94,96,97,98,100Mo, 110Pd, 159Tb(p, xn), E=25 MeV; 90,91,92,94Zr(p, xn), E=18 MeV; measured inclusive σ(En, θn); deduced precompound reaction single particle effects.
doi: 10.1103/PhysRevC.30.1480
1983HA33 Phys.Rev. C28, 1934 (1983) L.F.Hansen, S.M.Grimes, C.H.Poppe, C.Wong Charge Exchange (p, n) Reactions to the Isobaric Analog States of High Z Nuclei: 73 ≤ Z ≤ 92 NUCLEAR REACTIONS 181Ta, 197Au, 209Bi, 232Th, 238U(p, n), E=27 MeV; measured σ(En), σ(θ). 232Th, 238U(p, p), (p, n), E=26 MeV; measured σ(θ). 181Ta, 197Au, 209Bi(n, n), E=8.05 MeV; 232Th(n, n), E=7 MeV; 238U(n, n), E=6.44, 7 MeV; analyzed σ(θ); deduced Lane potential validity. 181W, 197Hg, 209Po, 232Pa, 238Np deduced IAS excitation. Coupled-channels calculations.
doi: 10.1103/PhysRevC.28.1934
1983SC19 Z.Phys. A311, 323 (1983) W.Scobel, L.F.Hansen, B.A.Pohl, C.Wong, M.Blann Double Differential Cross Sections for (p, xn) Reactions of 64Zn, 65Cu and 89Y with 26 MeV Protons NUCLEAR REACTIONS 64Zn, 65Cu, 89Y(p, xn), E=26 MeV; measured inclusive σ(θn, En). Tof. Preequilibrium, hybrid model analysis.
doi: 10.1007/BF01415688
1982BL19 Phys.Rev. C26, 1471 (1982) M.Blann, D.Akers, T.A.Komoto, F.S.Dietrich, L.F.Hansen, J.G.Woodworth, W.Scobel, J.Bisplinghoff, B.Sikora, F.Plasil, R.L.Ferguson Saturation Analysis as a Test of Statistical Fission in Heavy Ion Reactions NUCLEAR REACTIONS 120,122Sn(56Fe, X), E=330-456 MeV; measured σ(evaporation residue θ), σ(fragment θ) vs mass; deduced statistical fission decay yield limit. 176Os deduced fission barrier vs J.
doi: 10.1103/PhysRevC.26.1471
1982HA02 Phys.Rev. C25, 189 (1982) L.F.Hansen, I.D.Proctor, D.W.Heikkinen, V.A.Madsen Nuclear Deformation in the Actinide Region by Proton Inelastic Scattering NUCLEAR REACTIONS 232Th, 238U(p, p), (p, p'), E=26 MeV; measured σ(θ); deduced potential multipole moments. 232Th, 238U deduced β2, β4. Coupled-channels analysis.
doi: 10.1103/PhysRevC.25.189
1979HA54 Nucl.Sci.Eng. 72, 35 (1979) L.F.Hansen, C.Wong, T.T.Komoto, B.A.Pohl, E.Goldberg, R.J.Howerton, W.M.Webster Neutron and Gamma-Ray Spectra from 232Th, 235U, 238U, and 239Pu after Bombardment with 14-MeV Neutrons NUCLEAR REACTIONS 232Th, 235,238U, 239Pu(n, n), (n, γ), E=14 MeV; measured σ(En, Eγ). Leakage spectra from pulsed spheres, tof, electron recoil technique.
doi: 10.13182/NSE79-A19307
1978HA33 Phys.Rev. C18, 1582 (1978) L.F.Hansen, F.S.Dietrich, R.P.Koopman Identification of the Lowest 3- Collective Level in 116Cd NUCLEAR REACTIONS 116Cd(p, p'γ), E=5-20 MeV; measured σ(E, Eγ). 116Cd deduced levels, J, π.
doi: 10.1103/PhysRevC.18.1582
1977HA25 Nucl.Sci.Eng. 62, 550 (1977) L.F.Hansen, T.Komoto, E.F.Plechaty, B.A.Pohl, G.S.Sidhu, C.Wong Measurements and Calculations of the Electron Recoil Spectra from Gamma Rays Emitted by Nitrogen for a 14-MeV Neutron Source NUCLEAR REACTIONS N(n, X), E=14 MeV; measured electron recoil spectra.
doi: 10.13182/NSE77-A26991
1976DI13 Nucl.Sci.Eng. 61, 267 (1976) F.S.Dietrich, L.F.Hansen, R.P.Koopman Cross Section for the 9Be(n, t1)7Li Reaction between 13.3 and 15 MeV NUCLEAR REACTIONS 9Be(n, t), E=13.3-15 MeV; measured σ(E).
doi: 10.13182/NSE76-A27361
1976HA54 Nucl.Sci.Eng. 61, 201 (1976) L.F.Hansen, S.M.Grimes, R.J.Howerton, J.D.Anderson Calculations of the Neutron Emission Spectra from Materials Bombarded with 14-MeV Neutrons NUCLEAR REACTIONS 27Al, Fe, Ni, Cu, Nb(n, xn), E=14 MeV; calculated σ.
doi: 10.13182/NSE76-A27353
1974DI14 Phys.Rev. C10, 1587 (1974) F.S.Dietrich, L.F.Hansen, R.P.Koopman Lifetimes of the First Two Excited States of 66Ga NUCLEAR REACTIONS 66Zn(p, nγ), E=7.5-10 MeV; measured Eγ, γ(t). 66Ga levels deduced T1/2. Enriched target.
doi: 10.1103/PhysRevC.10.1587
1974HA42 Phys.Rev. C10, 1111 (1974) L.F.Hansen, J.C.Davis, F.S.Dietrich, M.C.Gregory, R.P.Koopman Levels of 64Ga via the 64Zn(p, n) and 64Zn(p, nγ) Reactions NUCLEAR REACTIONS 64Zn(p, n), E=10, 10.5 MeV; measured σ(En, θ). 64Zn(p, nγ), E=8.0-10.5 MeV; measured σ(E, Eγ), γ(t); deduced Q. 64Ga deduced levels, T1/2, J, π.
doi: 10.1103/PhysRevC.10.1111
1973HA54 Phys.Rev. C8, 2072 (1973) L.F.Hansen, S.M.Grimes, J.L.Kammerdiener, V.A.Madsen Analysis of Inelastic Proton Scattering from 14N between 8.60 and 26.0 MeV NUCLEAR REACTIONS 14N(p, p), (p, p'), E=8.6, 10.6, 12.6, 14.6 MeV; measured σ(E, θ); θ=15-165°; coupled-channel analysis. 14N(p, p'), E=18, 21, 23, 26 MeV, previous data compared with coupled-channel calculation.
doi: 10.1103/PhysRevC.8.2072
1971HA45 Phys.Rev. C4, 1189 (1971) L.F.Hansen, J.L.Kammerdiener, M.S.Weiss Analysis of the Scattering of 24-MeV 3He Particles from the Even Isotopes of Zinc NUCLEAR REACTIONS 64,66,68,70Zn(3He, 3He), (3He, 3He'), E=24 MeV; measured σ(θ); deduced optical model parameters. 64,66,68,70Zn deduced deformation parameters.
doi: 10.1103/PhysRevC.4.1189
1968HA30 Phys.Rev. 174, 1155 (1968) L.F.Hansen, M.L.Stelts, J.G.Vidal, J.J.Wesolowski, V.A.Madsen Study of the Two-Body Force Through the (He3, t) Charge-Exchange Reaction on O17 and O18 NUCLEAR REACTIONS 17,18O(3He, t), E=17.3 MeV; measured σ(Et, θ).
doi: 10.1103/PhysRev.174.1155
1968WE09 Phys.Rev. 172, 1072 (1968) J.J.Wesolowski, L.F.Hansen, M.L.Stelts Two-Particle, Two-Hole States in 40K from the Study of the 40Ar(3He, 3H)40K Reaction NUCLEAR STRUCTURE 40K; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.172.1072
1967HA14 Nucl.Phys. A98, 25(1967) L.F.Hansen, J.D.Anderson, J.W.McClure, B.A.Pohl, M.L.Stelts, J.J.Wesolowski, C.Wong The (α, n) Cross Sections on 17O and 18O Between 5 and 12.5 MeV NUCLEAR REACTIONS 17O, 18O(α, n), E = 5 to 12 MeV; measured σ(E), σ(E; En, θ). Enriched targets.
doi: 10.1016/0375-9474(67)90895-0
1967HA23 Phys.Rev. 158, 917 (1967) L.F.Hansen, H.F.Lutz, M.L.Stelts, J.G.Vidal, J.J.Wesolowski Study of the (α, t) Reaction in F19 NUCLEAR STRUCTURE 20Ne, 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.158.917
1967LU04 Nucl.Phys. A95, 591(1967) H.F.Lutz, J.J.Wesolowski, L.F.Hansen, S.F.Eccles Study of the 22Ne(d, d)22Ne, 22Ne(d, p)23Ne, 22Ne(d, t)21Ne and 22Ne(p, d)21Ne Reactions NUCLEAR REACTIONS 22Ne(d, d), (d, p), (d, t), E = 12.1 MeV; 22Ne(p, d), E = 18.2 MeV; measured σ(Ed, θ), σ(Ep, θ), σ(Et, θ). 21,22,23Ne deduced S, deformation parameters. Enriched target.
doi: 10.1016/0375-9474(67)90852-4
1967LU05 Nucl.Phys. A101, 241(1967) H.F.Lutz, J.J.Wesolowski, S.F.Eccles, L.F.Hansen Study of the 18O(p, t)16O and 18O(p, d)17O Reactions at E = 18.2 MeV NUCLEAR REACTIONS 18O(p, t), 18O(p, d), E=18.2 MeV; measured σ(Et, θ), σ(Ed, θ). 16,17O deduced levels, S. Enriched target.
doi: 10.1016/0375-9474(67)90185-6
1966HA13 Phys.Rev. 143, 800 (1966) L.F.Hansen, M.L.Stelts, J.J.Wesolowski Ground-State (p, n) Reactions in Mirror Nuclei and the Quasielastic Model of (p, n) Reactions NUCLEAR STRUCTURE 31S, 29P, 27Si; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.143.800
1966LU03 Phys.Letters 20, 410 (1966) H.F.Lutz, J.J.Wesolowski, L.F.Hansen, S.F.Eccles Excitation of the Ground State Band of 19F by 13.9 MeV Proton Scattering NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90763-3
1966WE04 Phys.Rev. 148, 1063 (1966) J.J.Wesolowski, L.F.Hansen, J.G.Vidal, M.L.Stelts Two-Nucleon Distorted-Wave Born Approximation Analysis of F19(d, α)O17 Data NUCLEAR STRUCTURE 19F, 17O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.148.1063
1965HA02 Bull.Am.Phys.Soc. 10, No.1, 25, BC1 (1965) Ground-State (p, n) Reactions in Mirror Nuclei and the Quasielastic Model of (p, n) Reactions NUCLEAR STRUCTURE 27Si, 29P, 31S; measured not abstracted; deduced nuclear properties.
1965WE05 Nucl.Phys. 71, 586(1965) J.J.Wesolowski, J.D.Anderson, L.F.Hansen, C.Wong, J.W.McClure Energy Levels of 31S and 19Ne NUCLEAR REACTIONS 31P(p, n), 19F(p, n), E = 7.5-13.0 MeV; measured σ(E;En, θ), Q. 31S, 19Ne deduced levels.
doi: 10.1016/0029-5582(65)90767-4
1964HA55 Phys.Rev. 136, B1000 (1964) (α, n) Reactions in Some Elements in the Region of A=100 NUCLEAR REACTIONS 89Y, 93Nb, 103Rh, Ag, 109Ag, 115In(α, n), E=10-20 MeV; measured reaction products, En, In; deduced σ(θ), σ. Comparison with available data.
doi: 10.1103/PhysRev.136.B1000
1963HA13 Bull.Am.Phys.Soc. 8, No.4, 304, D13 (1963) N15(p, n)O15 Reaction from 3.95-8.99 MeV NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.
1963HA46 Phys.Rev. 132, 1123 (1963) N15(p, n)O15 Ground-State Reactions and the Quasielastic Model of (p, n) Reactions NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.132.1123
1962HA13 Nuclear Phys. 30, 389 (1962) L.F.Hansen, R.C.Jopson, H.Mark, C.D.Swift Ta181(p, n)W181 and Au197(p, n)Hg197 Excitation Functions between 4 and 13 MeV NUCLEAR STRUCTURE 181W, 197Hg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90062-7
1962HA53 Phys.Rev. 128, 291 (1962) Statistical Theory Predictions For 5 to 11 MeV (p, n And (p, p'`) Nuclear Reactions in V51, Co59, Cu63, Cu65, and Rh103 NUCLEAR REACTIONS 51V(p, n), 59Co(p, n), 63Cu(p, n), 65Cu(p, n), 103Rh(p, n), E=5-11 MeV; measured products, 51Cr, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry B0066.
doi: 10.1103/PhysRev.128.291
1961AL33 Phys.Rev.Lett. 6, 13 (1961) 10-MeV proton reaction cross sections for Cu63 and Cu65 NUCLEAR REACTIONS 63Cu(p, n), 65Cu(p, n), E=9.8 MeV; measured products, En, In; deduced σ, σ(E). Data were imported from EXFOR entry C2006.
doi: 10.1103/PhysRevLett.6.13
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