NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.E.Evans Found 50 matches. 2005AH03 Phys.Rev. C 71, 054305 (2005) I.Ahmad, F.G.Kondev, E.F.Moore, M.P.Carpenter, R.R.Chasman, J.P.Greene, R.V.F.Janssens, T.Lauritsen, C.J.Lister, D.Seweryniak, R.W.Hoff, J.E.Evans, R.W.Lougheed, C.E.Porter, L.K.Felker Energy levels of 249Bk populated in the α decay of 25399Es and β- decay of 24996Cm RADIOACTIVITY 253Es(α); measured Eα, Eγ, γγ-, αγ-coin. 249Cm(β-) [from 248Cm(n, γ)]; measured Eγ, Iγ. 249Bk deduced levels, J, π, configurations, B(λ), g factors. 253Es(SF); measured Eγ, Iγ from fission fragment decay; deduced fission branching ratio. Gammasphere array, comparisons with model predictions.
doi: 10.1103/PhysRevC.71.054305
1981LO15 J.Inorg.Nucl.Chem. 43, 2239 (1981) R.W.Lougheed, E.K.Hulet, J.F.Wild, B.J.Qualheim, J.E.Evans, R.J.Dupzyk Two New Isotopes with N = 157: 256Es and 255Cf RADIOACTIVITY 256Es, 255Cf [from neutron irradiation of 255Es, 254Cf]; measured β-decay T1/2. NUCLEAR REACTIONS 255Es, 254Cf(n, γ), E=reactor; measured σ(effective); deduced evidence for 256Es, 255Cf. Enriched targets.
doi: 10.1016/0022-1902(81)80239-4
1971HO16 Nucl.Phys. A169, 641 (1971) R.W.Hoff, E.K.Hulet, R.J.Dupzyk, R.W.Lougheed, J.E.Evans Alpha Decay of 255Md, 256Md and 257Md RADIOACTIVITY 255,256,257Md [from 253,254Es(α, xn)]; measured T1/2, Eα, Iα; deduced hindrance factors, α/(α+EC) ratios, lower limit T1/2(SF). 253Es(α, n), (α, 2n), 254Es(α, n), E = 38 MeV; measured relative σ.
doi: 10.1016/0375-9474(71)90708-1
1971HU03 Phys.Rev. Lett. 26, 523 (1971) E.K.Hulet, J.F.Wild, R.W.Lougheed, J.E.Evans, B.J.Qualheim, M.Nurmia, A.Ghiorso Spontaneous-Fission Half-Life of 258Fm and Nuclear Instability RADIOACTIVITY, Fission 258Fm(SF)[from 257Fm(d, p)]; measured T1/2.
doi: 10.1103/PhysRevLett.26.523
1970HU17 UCRL-72858 (1970) E.K.Hulet, J.F.Wild, R.W.Lougheed, J.E.Evans, B.J.Qualheim, M.Nurmia, A.Ghiorso Spontaneous-Fission Half-Life of 258Fm and Nuclear Instability
1969EN03 Phys.Letters 30B, 476 (1969) J.B.A.England, R.G.Harris, L.H.Watson, D.H.Worledge, J.E.Evans Polarization of 3He Particles Elastically Scattered by 12C Nuclei NUCLEAR REACTIONS 12C(3He, 3He), E = 31.6 MeV; measured polarization P; deduced optical model spin-orbit potential.
doi: 10.1016/0370-2693(69)90176-2
1968AU07 Nucl.Phys. A112, 329 (1968) G.F.Auchampaugh, C.D.Bowman, J.E.Evans Neutron-Induced Fission Cross Sections Of 232U NUCLEAR REACTIONS 232U(n, n), (n, f), E=-0.6 eV-1.9 keV; measured products; deduced resonance parameters, σ, σ(E). Data were imported from EXFOR entry 12383.
doi: 10.1016/0375-9474(68)90205-4
1968HO13 Nucl.Phys. A115, 225 (1968) R.W.Hoff, J.E.Evans, E.K.Hulet, R.J.Dupzyk, B.J.Qualheim Nuclear Decay Properties of 256Fm RADIOACTIVITY 256Fm [from 253Es(α, p), 253Es(α, n)256Md EC]; measured T1/2, Eα, Iα. Reactor-produced target. Isotopically enriched 256Fm. NUCLEAR REACTIONS 255Fm(n, γ), E = reactor spectrum; measured σ. Reactor-produced target.
doi: 10.1016/0375-9474(68)90657-X
1968HO15 Bull.Am.Phys.Soc. 13, No.4, 604, DF6 (1968); Oral Report R.W.Hoff, E.K.Hulet, R.J.Dupzyk, R.W.Lougheed, J.E.Evans Alpha Decay of 255Md, 256Md, and 257Md NUCLEAR STRUCTURE 256Md, 257Md, 255Md; measured not abstracted; deduced nuclear properties.
1968HU06 Bull.Am.Phys.Soc. 13, No.4, 604, DF7 (1968); Oral Report E.K.Hulet, A.Ghiorso, R.W.Lougheed, J.E.Evans, J.D.Brady, R.W.Hoff, R.E.Stone, B.J.Qualheim Discovery of 258Md NUCLEAR STRUCTURE 258Md; measured not abstracted; deduced nuclear properties.
1968WO07 J.Opt.Soc.Am. 58, 998 (1968) E.F.Worden, R.G.Gutmacher, R.W.Lougheed, J.E.Evans, J.G.Conway Hyperfine Structure in the 253Es Emission Spectrum NUCLEAR STRUCTURE 253Es; measured not abstracted; deduced nuclear properties.
doi: 10.1364/JOSA.58.000998
1967CU01 Phys.Letters 24B, 399 (1967) Levels in 33P NUCLEAR STRUCTURE 33P; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90303-6
1966FU13 Phys.Rev. 152, 1046 (1966) S.C.Fultz, J.T.Caldwell, B.L.Berman, R.L.Bramblett, M.A.Kelly, H.D.Wilson, M.S.Coops, R.W.Lougheed, J.E.Evans, R.W.Hoff Measurement of the Average Neutron Yield Per Fission for Am-242m NUCLEAR REACTIONS, Fission 233,235U, 242Am(n, F), E = thermal; measured neutrons/fission.
doi: 10.1103/PhysRev.152.1046
1966HO01 Phys.Rev. 148, 1192 (1966); See keynumber 1966RG01 R.W.Hoff, C.P.Bailey, G.W.Barton, G.H.Coleman, M.S.Coops, J.E.Evans, B.A.Hannon, W.N.Hayes, R.A.Heckman, E.K.Hulet, R.W.Lougheed, R.J.Morrow, R.S.Newbury, B.J.Qualheim, R.Quong, E.H.Stearns, H.D.Wilson, J.P.Balagna, J.W.Barnes, G.A.Cowan, W.R.Daniels, B.J.Dropesky, G.P.Ford, J.S.Gilmore, S.B.Helmick, D.C.Hoffman, J.D.Knight, G.W.Knobeloch, C.J.Orth, T.T.Shull, H.L.Smith, W.G.Warren, K.Wolfsberg, F.Asaro, J.Burnett, B.B.Cunningham, S.M.Fried, J.T.Haley, A.Ghiorso, J.Green, R.Latimer, F.T.McCarthy, H.V.Michel, M.C.Michel, D.F.Mosier, T.C.Parsons, I.Perlman, J.E.Rees, J.C.Wallmann, R.F.Barnes, L.J.Basile, H.Diamond, P.R.Fields, A.M.Friedman, E.P.Horowitz, J.K.Lerner, D.N.Metta, J.Milsted, R.K.Sjoblom, C.M.Stevens Nuclear Decay Properties of Heavy Nuclides Produced in Thermonuclear Explosions - Par and Barbel Events RADIOACTIVITY 251,252,253,254Cf, 255Es, 257,258Fm(α), 250Cm(SF), 251Bk, 252Cm(β-) [from U(n, F), U(n, X), E ∼ 2 MeV]; measured decay products, Eα, Iα; deduced α-particles energies, α-decay branchings, T1/2. Two low-yield thermonuclear explosions, the Par and Barbel events, chemical separation of products. NUCLEAR REACTIONS Cm(n, X)249Cf/250Cf/252Cf/252Cf/253Cf/254Cf/253Es/254Es/255Es, E thermal; measured reaction products, Eα, Iα, Eβ, Iβ; deduced isotopic abundances. Cm irradions, reactor.
doi: 10.1103/PhysRev.148.1192
1964HU02 Phys.Rev.Letters 13, 343 (1964) E.K.Hulet, R.W.Hoff, J.E.Evans, R.W.Lougheed 79-Day Fermium Isotope of Mass 257 NUCLEAR STRUCTURE 257Fm; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.13.343
1963BE20 Proc.Third Conf.on Reactions between Complex Nuclei, Asilomar, Cal., A.Ghiorso, R.M.Diamond, H.E.Conzett, Ed., Univ.of California, p.417 (1963) R.D.Bent, J.E.Evans, G.C.Morrison, I.J.Van Heerden Lifetimes of Levels in Ne21 NUCLEAR STRUCTURE 21Ne; measured not abstracted; deduced nuclear properties.
1963BE41 Conf.Low Medium Energy Nucl.Phys., Univ.Manchester, p. 9 (1963) R.D.Bent, J.E.Evans, G.C.Morrison, I.J.Van Heerden Lifetimes of Levels in Ne21 NUCLEAR STRUCTURE 21Ne; measured not abstracted; deduced nuclear properties.
1963EV03 Phys.Rev. 131, 818 (1963) J.E.Evans, J.A.Kuehner, A.E.Litherland, E.Almqvist Spin-Parity Combinations for Levels in Mg24 and Si28 NUCLEAR STRUCTURE 28Si, 24Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.131.818
1963EV04 Phys.Rev. 131, 1632 (1963) J.E.Evans, J.A.Kuehner, E.Almqvist Study of the C12(d, p)C13 Reaction Mechanism; Polarization and (d, pγ) Correlations NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.131.1632
1963EV05 Phys.Rev. 131, 1642 (1963) Proton Polarization in the Reaction O16(d, p)O17 (0.87 Mev) NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.131.1642
1962AL07 Phys.Can. 18, No.3, 40, 10.3 (1962) E.Almqvist, J.E.Evans, J.A.Kuehner Studies of the Polarization of Protons from (d, p) Stripping Reactions NUCLEAR STRUCTURE 29Si, 12C, 16O; measured not abstracted; deduced nuclear properties.
1962EV01 Bull.Am.Phys.Soc. 7, No.1, 60, R12 (1962) J.E.Evans, J.A.Kuehner, E.Almqvist Polarization in the C12(d, p) Reaction NUCLEAR STRUCTURE 12C, 13C; measured not abstracted; deduced nuclear properties.
1962EV02 AECL-1542, p.11 (1962) J.E.Evans, J.A.Kuehner, E.Almqvist Polarization Studies of C12(d, p)C13* NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1962EV03 AECL-1542, p.13 (1962) Polarization of Protons from the Reaction O16(d, p)O17* (0.87 MeV) NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
1962EV04 Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 15, 5.9 (September 1962) J.E.Evans, J.A.Kuehner, E.Almqvist NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1962KU01 Bull.Am.Phys.Soc. 7, No.1, 73, V12 (1962) J.A.Kuehner, A.E.Litherland, E.Almqvist, J.E.Evans Parity Determinations for States of Mg24 and Si28 NUCLEAR STRUCTURE 28Si, 24Mg; measured not abstracted; deduced nuclear properties.
1962SI17 Nucl.Sci.Eng. 12, 243 (1962) F.B.Simpson, W.H.Burgus, J.E.Evans, H.W.Kirby Total Neutron Cross Section of Pa231
doi: 10.13182/NSE62-A26064
1961EV03 Nuclear Phys. 27, 41 (1961) Polarization in C12(p, p) Scattering from 5 to 10.5 MeV
doi: 10.1016/0029-5582(61)90489-8
1961EV04 AECL-1408, p.13 (1961) J.E.Evans, J.A.Kuehner, E.Almqvist Polarization in (d, p) Reactions NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1961EV05 AECL-1472, p.14 (1961) J.E.Evans, J.A.Kuehner, E.Almqvist Measurements of Proton Polarization and (p, γ) Angular Correlations in the Reaction C12(d, pγ)C13 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1961JO21 Nuclear Sci. And Eng. 11, 298 (1961) E.G.Joki, J.E.Evans, R.R.Smith Total Slow Neutron Cross Section Measurements of Titanium, Zirconium, and Hafnium NUCLEAR STRUCTURE Hf, Zr, Ti; measured not abstracted; deduced nuclear properties.
doi: 10.13182/NSE61-A26007
1961KU12 AECL-1408, p.10 (1961) J.A.Kuehner, A.E.Litherland, E.Almqvist, J.E.Evans Parity Determinations from Angular Distributions in O16(C12, α)Mg24 and O16(O16, α)Si28 NUCLEAR STRUCTURE 16O, 24Mg, 28Si; measured not abstracted; deduced nuclear properties.
1961MO15 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.575 (1961) G.C.Morrison, A.T.G.Ferguson, J.E.Evans Angular Distributions of the Be9(d, n)B10 Neutrons NUCLEAR STRUCTURE 9B; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0096. 1961PA01 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.313 (1961) E.B.Paul, J.E.Evans, J.H.Montague The 2.2 MeV Level in Al27 NUCLEAR STRUCTURE 27Si; measured not abstracted; deduced nuclear properties.
1960EV02 Nuclear Phys. 15, 646 (1960) Polarization in C12(pp) Scattering NUCLEAR STRUCTURE 12C, 13N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90362-X
1960EV03 Nuclear Sci. And Eng. 8, 66 (1960) Evaluation of Low-Energy Cross Section Data for U233
doi: 10.13182/NSE8-1-66
1959EV81 Bull.Am.Phys.Soc. 4, No.4, 270, SA2 (1959) J.E.Evans, F.W.Firk, B.B.Kinsey, M.C.Moxon, J.R.Waters, G.H.Williams Analysis of the Low-Energy Neutron Resonances in Tungsten Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21317. 1959EV82 Can.J.Phys. 37, 396 (1959) J.E.Evans, B.B.Kinsey, B.G.Whitmore Measurement of the Energies of Nuclear States Excited by Inelastic Neutron Scattering, and a Search for Electric Monopole Transitions in Pb
doi: 10.1139/p59-044
1959SI86 Bull.Am.Phys.Soc. 4, No.7, 414, J9 (1959) F.B.Simpson, W.H.Burgus, O.D.Simpson, J.E.Evans Total Neutron Cross Section of Pa231
1959WA06 Nuclear Phys. 12, 563 (1959) J.R.Waters, J.E.Evans, B.B.Kinsey, G.H.Williams Spins and Radiation Widths of the Low Energy Neutron Resonances in Tungsten
doi: 10.1016/0029-5582(59)90098-7
1958EV82 Nuclear Phys. 9, 205 (1958) J.E.Evans, B.B.Kinsey, J.R.Waters, G.H.Williams Radiation Widths of Neutron Resonances in Ta
doi: 10.1016/0029-5582(58)90392-4
1958FL41 Proc.U.N.Intern.Conf.Peaceful Uses At. Energy, 2nd, Geneva 15, 111 (1958) R.G.Fluharty, M.S.Moore, J.E.Evans
1957SM79 Phys.Rev. 107, 525 (1957) M.S.Smith, R.R.Smith, E.G.Joki, J.E.Evans Neutron Total Cross Section Of Np237 From 0.02 To 2.8 Ev NUCLEAR REACTIONS 237Np(n, X), 237Np(n, n), 237Np(n, x), E=0.02016-2.876 eV; measured products; deduced resonance parameters, σ, σ(E). Data were imported from EXFOR entry 12487.
doi: 10.1103/PhysRev.107.525
1956BR99 Phys.Rev. 104, 1054 (1956) R.M.Brugger, J.E.Evans, E.G.Joki, R.S.Shankland Total Neutron Cross Section of Chlorine and Carbon NUCLEAR REACTIONS C, Cl(n, X), E=0.03-15000 eV; measured total σ. 35Cl deduced resonance energy, width, J.
doi: 10.1103/PhysRev.104.1054
1956JO36 Phys.Rev. 103, 1326 (1956) Total Neutron Cross Section Of Thulium In The Energy Region 0.038 To 1.56Ev NUCLEAR REACTIONS 169Tm(n, x), E=0.0253-1.585 eV; measured products ; deduced σ, σ(E). Data were imported from EXFOR entry 12111.
doi: 10.1103/PhysRev.103.1326
1955EV24 Phys.Rev. 97, 565 (1955) J.E.Evans, E.G.Joki, R.R.Smith Evidence for a second naturally occuring isotope in tantalum NUCLEAR REACTIONS Ta(n, x), 180Ta(n, n), 180Ta(n, x), E=0.02531-82.16 eV; measured products; deduced σ, σ(E), resonance parameters. Data were imported from EXFOR entry 12183.
doi: 10.1103/PhysRev.97.565
1949BO67 Phys.Rev. 75, 1401 (1949) T.W.Bonner, J.E.Evans, J.C.Harris, G.C.Phillips The Neutrons and Gamma-Rays from the Disintegration of C12 by Deutrons
doi: 10.1103/PhysRev.75.1401
1949WH01 Phys.Rev. 75, 688 (1949) W.Whaling, J.E.Evans, T.W.Bonner Neutrons from Deuteron Bombardment of Li6 NUCLEAR REACTIONS 6,7Li(d, X), E=0.25-2.2 MeV; measured reaction products, En, In; deduced relative neutron yields.
doi: 10.1103/PhysRev.75.688
1948BO20 Phys.Rev. 73, 885 (1948) T.W.Bonner, J.E.Evans, C.W.Malich, J.R.Risser A Study of the Breakup of Li8
doi: 10.1103/PhysRev.73.885
1948BO21 Phys.Rev. 73, 666 (1948) Resonances in the disintegration of fluorine and lithium by protons NUCLEAR REACTIONS 7Li(p, γ), 19F(p, γ), E=334 keV-1.3 MeV; measured products, 20Ne, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry A1406.
doi: 10.1103/PhysRev.73.666
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