NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.W.Lees Found 23 matches. 1982ED01 Ann.Nucl.Energy 9, 127 (1982) G.Edwards, D.J.S.Findlay, E.W.Lees Measurements of Prompt ν-Bar and Variance for the Spontaneous Fission of 252Cf and 242Pu RADIOACTIVITY, Fission 252Cf(SF), 242Pu(SF); measured prompt neutron multiplicity average, variance distributions.
doi: 10.1016/0306-4549(82)90012-3
1981ED01 Ann.Nucl.Energy 8, 105 (1981) G.Edwards, D.J.S.Findlay, E.W.Lees Improvements in the Description of the Multiplicities of the Prompt Neutrons Emitted in Fission RADIOACTIVITY, Fission 242,240Pu, 252Cf(SF); calculated prompt neutron multiplicity distributions. Truncated renormalized Gaussian, truncated renormalized double Gaussian treatments. NUCLEAR REACTIONS, Fission 235U, 239Pu(n, F), E not given; calculated prompt neutron multiplicity distribution. Truncated renormalized Gaussian, truncated renormalized double Gaussian treatments.
doi: 10.1016/0306-4549(81)90107-9
1979LE15 J.Phys.(London) G5, 1307 (1979) E.W.Lees, B.H.Patrick, S.Lindley The 238U(γ, α) and 238U(n, αn') Reactions - Have They Really Been Observed (Question) NUCLEAR REACTIONS 238U(γ, α), E=15.5 MeV; 238U(n, n'α), E=14.7 MeV; measured upper limit for σ(E).
doi: 10.1088/0305-4616/5/9/013
1979LE16 J.Phys.(London) G5, 1307 (1979) E.W.Lees, B.H.Patrick, S.Lindley The 238U(γ, α) and 238U(n, αn') Reactions--Have They Really Been Observed (Question) NUCLEAR REACTIONS 238U(γ, α), E=15.5 MeV; 238U(n, αn'), E=14.7 MeV; measured upper limit for σ(E).
doi: 10.1088/0305-4616/5/9/013
1978AR07 J.Phys.(London) G4, 961 (1978) R.G.Arthur, R.P.Singhal, S.W.Brain, W.A.Gillespie, A.Johnston, E.W.Lees, M.W.S.Macauley Vibrational States in 108Pd Studied by Elastic and Inelastic Electron Scattering NUCLEAR REACTIONS 108Pd(e, e), E=21-121 MeV; measured σ(E). 108Pd levels deduced form factors, quadrupole moment, B(λ).
doi: 10.1088/0305-4616/4/6/023
1978LE24 Ann.Nucl.Energy 5, 133 (1978) Neutron Production from (α, n) Reactions in 241AmO2 NUCLEAR REACTIONS 241Am(α, n), E < 5.486 MeV [from 241Am decay]; measured yield.
doi: 10.1016/0306-4549(78)90065-8
1977BR16 J.Phys.(London) G3, 821 (1977) S.W.Brain, A.Johnstons, W.A.Gillespie, E.W.Lees, R.P.Singhal The Ground-State Charge Distribution of the Silicon Isotopes and the Excited States of 28Si, 30Si NUCLEAR REACTIONS 28,29,30Si(e, e'), E=18.5-117.1 MeV; measured σ(E, θ). 28,30Si deduced rms radii, B(λ). 29Si deduced rms radii.
doi: 10.1088/0305-4616/3/6/013
1977BR35 J.Phys.(London), G3, 681 (1977) S.W.Brain, A.Johnston, W.A.Gillespie, E.W.Lees, R.P.Singhal Inelastic Electron Scattering from 29Si NUCLEAR REACTIONS 29Si(e, e'), E=63-117 MeV; measured σ(E;θ). 29Si deduced levels, B(λ). Enriched target, resolution=0.16%, DWBA analysis.
doi: 10.1088/0305-4616/3/5/014
1977GI13 J.Phys.(London) G3, L-169 (1977) W.A.Gillespie, M.W.S.Macauley, A.Johnston, E.W.Lees, R.P.Singhal B(E2) and Q21+ Measurements in the Even-Mass Cd Isotopes NUCLEAR REACTIONS 110,112,114,116Cd(e, e'), E=68, 112 MeV; measured σ(θ). 110,112,114,116Cd deduced quadrupole moment, B(E2). Separated targets, resolution 0.15%, DWBA analysis, anharmonic vibrational model.
doi: 10.1088/0305-4616/3/8/005
1977MA42 J.Phys.(London) G3, 1717 (1978) M.W.S.Macauley, R.P.Singhal, R.G.Arthur, S.W.Brain, W.A.Gillespie, A.Johnston, E.W.Lees, A.G.Slight An Experimental and Theoretical Study of the Low-Lying States of 15N NUCLEAR REACTIONS 15N(e, e'), E=60-120 MeV; measured σ(E, θ). 15N deduced form factors, B(λ). Separated isotope gas target. Shell model, DWBA analysis.
doi: 10.1088/0305-4616/3/12/011
1977SI02 Nucl.Phys. A279, 29 (1977) R.P.Singhal, A.Johnston, W.A.Gillespie, E.W.Lees Inelastic Scattering of Electrons from 27Al NUCLEAR REACTIONS 27Al(e, e'), E=62-112 MeV; measured σ. 27Al deduced B(E2), transition radius. Intermediate-coupling model, large-basis shell model.
doi: 10.1016/0375-9474(77)90418-3
1976GI07 J.Phys.(London) G2, 185 (1976) W.A.Gillespie, R.P.Singhal, S.W.Brain, A.Johnston, E.W.Lees Excitation of Vibrational States in 114Cd by Inelastic Electron Scattering NUCLEAR REACTIONS 114Cd(e, e'), E=68-112 MeV; measured σ(E, θ). 114Cd levels deduced form-factors, B(λ), quadrupole moment, β. Anharmonic model.
doi: 10.1088/0305-4616/2/3/010
1976LE07 J.Phys.(London) G2, 105 (1976) E.W.Lees, C.S.Curran, T.E.Drake, W.A.Gillespie, A.Johnston, R.P.Singhal Elastic Electron Scattering from the Stable Isotopes of Magnesium NUCLEAR REACTIONS 24,25,26Mg(e, e'), E=22.9-119.7 MeV; measured σ(E, θ). 24,25,26Mg deduced rms radii, form factors. DWBA analysis. Enriched targets.
doi: 10.1088/0305-4616/2/2/007
1976LE11 J.Phys.(London) G2, 341 (1976) E.W.Lees, C.S.Curran, T.E.Drake, W.A.Gillespie, A.Johnston, R.P.Singhal Inelastic Electron Scattering from 25Mg NUCLEAR REACTIONS 25Mg(e, e'), E=61.9-119.3 MeV; measured σ(E, θ). 25Mg levels deduced radial parameters, B(E2), form factors. DWBA analysis, Nilsson model comparison, enriched target.
doi: 10.1088/0305-4616/2/5/010
1976MA30 J.Phys.(London) G2, L35 (1976) M.W.S.Macauley, R.P.Singhal, R.G.Arthur, S.W.Brain, W.A.Gillespie, A.Johnston, E.W.Lees, A.G.Slight The 6.32 MeV Excitation in 15N: Is it a Single-Particle Transition (Question) NUCLEAR REACTIONS 15N(e, e'), E=60-120 MeV; measured σ(E, θ). 15N level deduced form factors, effective charge. DWBA, shell model analysis. Enriched target.
doi: 10.1088/0305-4616/2/3/004
1975LE02 J.Phys.(London) G1, L13 (1975) E.W.Lees, C.S.Curran, S.W.Brain, W.A.Gillespie, A.Johnston, R.P.Singhal The Ground State Band of 25Mg Studied by Electron Scattering NUCLEAR REACTIONS 25Mg(e, e'), E=61.9-119.3 MeV; measured σ(E, Ee', θ). 25Mg transitions deduced B(E2).
doi: 10.1088/0305-4616/1/2/001
1975SI21 J.Phys. (London) G1, 558 (1975) R.P.Singhal, S.W.Brain, C.S.Curran, W.A.Gillespie, A.Johnston, E.W.Lees, A.G.Slight Inelastic Scattering of Electrons from 90Zr NUCLEAR REACTIONS 90Zr(e, e'), E=53.75-112.2 MeV; measured σ(E, e', θ). 90Zr deduced levels, J, π, B(λ).
doi: 10.1088/0305-4616/1/5/008
1974LE17 J.Phys.(London) A7, 936 (1974) E.W.Lees, A.Johnston, S.W.Brain, C.S.Curran, W.A.Gillespie, R.P.Singhal The Study of the Excited States of 26Mg below 11 MeV by Inelastic Electron Scattering NUCLEAR REACTIONS 26Mg(e, e'), E=56.89, 81.36, 82.75, 84.16, 85.09, 91.28, 95.74, 110.45, 110.71 MeV; measured σ(E, Ee', θ). 26Mg deduced levels, J, π, form factors β, B(λ), transition radii.
doi: 10.1088/0305-4470/7/8/005
1974SI01 Nucl.Phys. A218, 189 (1974) R.P.Singhal, S.W.Brain, W.A.Gillespie, A.Johnston, E.W.Lees, A.G.Slight The B(E2) and R(tr) of 2+1 States in 90Zr and 60Ni NUCLEAR REACTIONS 60Ni, 90Zr(e, e')E=45-250 MeV; measured σ. 60Ni, 90Zr levels deduced B(E2), transition radius.
doi: 10.1016/0375-9474(74)90030-X
1973LE17 J.Phys.(London) A6, L116 (1973) E.W.Lees, A.Johnston, S.W.Brain, C.S.Curran, W.A.Gillespie, R.P.Singhal The B(E2) Value of the First Excited State of 26Mg NUCLEAR REACTIONS 26Mg(e, e'); measured σ(θ). 26Mg level deduced B(E2).
doi: 10.1088/0305-4470/6/8/003
1973SI39 Nucl.Phys. A216, 29 (1973) R.P.Singhal, S.W.Brain, C.S.Curran, T.E.Drake, W.A.Gillespie, A.Johnston, E.W.Lees Elastic Scattering of Electrons from the N = 50 Isotones; 88Sr, 89Y, 90Zr and 92Mo NUCLEAR REACTIONS 88Sr, 89Y, 90Zr, 92Mo(e, e), E0=25-120 MeV; measured σ(E). Deduced nuclear charge distributions.
doi: 10.1016/0375-9474(73)90515-0
1972CU02 J.Phys.(London) A5, L39 (1972) C.S.Curran, T.E.Drake, A.Johnston, S.W.Brain, W.A.Gillespie, E.W.Lees, R.P.Singhal, A.G.Slight Nuclear Charge Distributions of the Isotopes 24Mg, 25Mg and 26Mg from Elastic Electron Scattering NUCLEAR REACTIONS 24,25,26Mg(e, e), E =not given; measured σ(θ). 24,25,26Mg deduced nuclear charge distributions.
doi: 10.1088/0305-4470/5/4/001
1971SI17 J.Phys.(London). A4, L93 (1971) R.P.Singhal, C.S.Curran, T.E.Drake, W.A.Gillespie, A.Johnston, E.W.Lees Nuclear Charge Distributions of 89Y, 90Zr and 92Mo by Elastic Electron Scattering NUCLEAR REACTIONS 89Y, 90Zr, 92Mo(e, e), E not given; measured σ(θ). 89Y, 90Zr, 92Mo deduced nuclear charge distributions.
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