NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Evans Found 94 matches. 2023AG06 Eur.Phys.J. C 83, 1117 (2023) X.Aguerre, R.Arnold, C.Augier, A.S.Barabash, A.Basharina-Freshville, S.Blondel, S.Blot, M.Bongrand, R.Breier, V.Brudanin, J.Busto, A.Bystryakov, A.J.Caffrey, C.Cerna, J.P.Cesar, M.Ceschia, E.Chauveau, A.Chopra, L.Dawson, D.Duchesneau, D.Durand, J.J.Evans, R.Flack, P.Franchini, X.Garrido, C.Girard-Carillo, B.Guillon, P.Guzowski, M.Hoballah, R.Hodak, P.Hubert, M.H.Hussain, S.Jullian, A.Klimenko, O.Kochetov, S.I.Konovalov, F.Konarik, T.Krizak, D.Lalanne, K.Lang, Y.Lemiere, P.Li, P.Loaiza, G.Lutter, M.Macko, F.Mamedov, C.Marquet, F.Mauger, A.Minotti, B.Morgan, I.Nemchenok, M.Nomachi, F.Nowacki, H.Ohsumi, G.Oliviero, V.Palusova, C.Patrick, F.Perrot, M.Petro, A.Pin, F.Piquemal, P.Povinec, S.Pratt, P.Pridal, W.S.Quinn, Y.A.Ramachers, A.Remoto, J.L.Reyss, C.L.Riddle, E.Rukhadze, R.Saakyan, A.Salamatin, R.Salazar, X.Sarazin, J.Sedgbeer, Yu.Shitov, L.Simard, F.Simkovic, A.Smetana, A.Smolnikov, S.Soldner-Rembold, I.Stekl, J.Suhonen, G.Szklarz, H.Tedjditi, J.Thomas, V.Timkin, V.I.Tretyak, V.I.Tretyak, V.I.Umatov, I.Vanushin, Y.Vereshchaka, V.Vorobel, D.Waters, F.Xie Measurement of the double-β-decay of 150Nd to the 0+1 excited state of 150Sm in NEMO-3 RADIOACTIVITY 150Nd(2β-); measured decay products, Eγ, Iγ, Eβ, Iβ; deduced T1/2, nuclear matrix elements for transitions to excited states. Comparison with available data. The NEMO-3 experiment in the Modane Underground Laboratory (LSM).
doi: 10.1140/epjc/s10052-023-12227-x
2021AR11 Phys.Rev. C 104, L061601 (2021) R.Arnold, C.Augier, A.S.Barabash, A.Basharina-Freshville, S.Blondel, S.Blot, M.Bongrand, D.Boursette, R.Breier, V.Brudanin, J.Busto, A.J.Caffrey, S.Calvez, C.Cerna, J.P.Cesar, M.Ceschia, A.Chapon, E.Chauveau, A.Chopra, L.Dawson, D.Duchesneau, D.Durand, G.Eurin, J.J.Evans, L.Fajt, D.Filosofov, R.Flack, P.Franchini, X.Garrido, C.Girard-Carillo, H.Gomez, B.Guillon, P.Guzowski, R.Hodak, A.Huber, P.Hubert, C.Hugon, M.H.Hussain, S.Jullian, A.Klimenko, O.Kochetov, S.I.Konovalov, V.Kovalenko, D.Lalanne, K.Lang, Y.Lemiere, T.Le Noblet, Z.Liptak, X.R.Liu, P.Loaiza, G.Lutter, M.Macko, C.Macolino, F.Mamedov, C.Marquet, F.Mauger, A.Minotti, B.Morgan, J.Mott, I.Nemchenok, M.Nomachi, F.Nova, F.Nowacki, H.Ohsumi, G.Oliviero, R.B.Pahlka, V.Palusova, C.Patrick, F.Perrot, A.Pin, F.Piquemal, P.Povinec, P.Pridal, W.S.Quinn, Y.A.Ramachers, A.Remoto, J.L.Reyss, C.L.Riddle, E.Rukhadze, R.Saakyan, A.Salamatin, R.Salazar, X.Sarazin, J.Sedgbeer, Yu.Shitov, L.Simard, F.Simkovic, A.Smetana, A.Smolnikov, S.Soldner-Rembold, B.Soule, I.Stekl, J.Suhonen, C.S.Sutton, G.Szklarz, H.Tedjditi, J.Thomas, V.Timkin, S.Torre, Vl.I.Tretyak, V.I.Tretyak, V.I.Umatov, I.Vanushin, C.Vilela, V.Vorobel, D.Waters, F.Xie Search for periodic modulations of the rate of double-β decay of 100Mo in the NEMO-3 detector RADIOACTIVITY 100Mo(2β-); measured two electrons in final state of 0νββ decay, decay rates and power spectra using NEMO-3 detector; searched for periodic modulations of double-β decay rate by Lomb-Scargle periodogram technique, and its error-weighted extension; deduced no evidence of modulations with amplitude greater than 2.5% at the 95% confidence level.
doi: 10.1103/PhysRevC.104.L061601
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
1999EL04 J.Phys.(London) G25, 667 (1999) J.P.Elliott, J.A.Evans, P.Halse Mappings from Shell-Model SU(3) to Boson SU(3)
doi: 10.1088/0954-3899/25/4/016
1999EL09 J.Phys.(London) G25, 2071 (1999) A Direct Mapping from Shell Model SU(3) to Boson SU(3)
doi: 10.1088/0954-3899/25/10/307
1997EV05 Nucl.Phys. A627, 71 (1997) J.A.Evans, V.S.Lac, J.P.Elliott A New Method for IBM3 Calculations
doi: 10.1016/S0375-9474(97)00590-3
1997LA12 Phys.Lett. 394B, 231 (1997) V.S.Lac, J.P.Elliott, J.A.Evans On the Validity of the O(18) Coupling Scheme in N ∼ Z Nuclei NUCLEAR STRUCTURE 62,64Zn, 64,66Ge, 68Se; calculated 0+, 2+, 3+, 4+ states, wave functions; deduced O(18) coupling scheme validity related features.
doi: 10.1016/S0370-2693(97)00027-0
1996AR31 Hyperfine Interactions 103, 169 (1996) D.S.Armstrong, J.Bauer, J.Evans, T.P.Gorringe, B.L.Johnson, S.Kalvoda, R.Porter, B.Siebels, E.Gete, D.F.Measday, B.A.Moftah, S.Stanislaus Muon Capture by Silicon 28 NUCLEAR REACTIONS 28Si(μ-, γ), E at rest; measured Eγ, Iγ; deduced nuclear recoil, γν-correlation coefficient.
1996EL02 Nucl.Phys. A597, 341 (1996) J.P.Elliott, J.A.Evans, V.S.Lac Electromagnetic Operators in IBM-3 and Their Dependence on the Boson Number and Isospin
doi: 10.1016/0375-9474(95)00475-0
1996EL10 Nucl.Phys. A609, 1 (1996) J.P.Elliott, J.A.Evans, V.S.Lac, G.L.Long An IBM-3 Analysis of the Nuclei Just Beyond the Magic Numbers N = Z = 28 NUCLEAR STRUCTURE 58,60,62,64Ni, 60,62,64,66Zn, 64,66,68Ge, 68Se; calculated binding energies, level spectra, B(λ). Isospin-invariant form of IBM-3.
doi: 10.1016/S0375-9474(96)00292-8
1995EV02 Nucl.Phys. A593, 85 (1995) J.A.Evans, J.P.Elliott, V.S.Lac, G.L.Long An IBM-3 Hamiltonian from a Multi-j-Shell Model
doi: 10.1016/0375-9474(95)00326-V
1995LA06 Nucl.Phys. A587, 101 (1995) V.S.Lac, J.P.Elliott, J.A.Evans, G.L.Long A Comparison of the IBM-1 Projections from IBM-2 and IBM-3
doi: 10.1016/0375-9474(94)00811-Z
1995SI19 Phys.Rev. C52, 1488 (1995) B.Siebels, T.P.Gorringe, W.P.Alford, J.Bauer, J.Evans, S.El-Kateb, K.P.Jackson, A.Trudel, S.Yen Gamow-Teller Strength in 23Na(n, p) and a Comparison to 23Na(μ-, ν) NUCLEAR REACTIONS 23Na(n, p), E=198 MeV; measured σ(θ). 23Ne levels deduced Gamow-Teller transition strength. Comparison with 23Na(μ-, ν) data.
doi: 10.1103/PhysRevC.52.1488
1994MO07 J.Phys.(London) G20, 787 (1994) D.S.Mosbah, J.A.Evans, W.D.Hamilton An IBA-2 Calculation of E2/M1 Multipole Mixing Ratios of Transitions in 182,184,186W NUCLEAR STRUCTURE 182,184,186W; calculated levels, B(λ), δ(E2/M1). Interacting boson approximation.
doi: 10.1088/0954-3899/20/5/012
1989AB13 Nucl.Phys. A503, 452 (1989) M.Abdelaziz, J.P.Elliott, M.J.Thompson, J.A.Evans On the Role of Isoscalar Bosons in Lighter Nuclei NUCLEAR STRUCTURE 46V, 48Cr, 46,44Ti, 44Sc; calculated levels, B(λ). 44Cr; calculated β-decay log ft. Shell model wave functions, boson analysis.
doi: 10.1016/0375-9474(89)90244-3
1989TH05 Nucl.Phys. A504, 436 (1989) M.J.Thompson, J.P.Elliott, J.A.Evans A Microscopic IBM2 Hamiltonian for Particle-Hole Systems NUCLEAR STRUCTURE 46Ti, 48Cr, 89,90Zr; calculated levels. Microscopic interacting boson model.
doi: 10.1016/0375-9474(89)90550-2
1988AB02 J.Phys.(London) G14, 219 (1988) M.Abdelaziz, M.J.Thompson, J.P.Elliott, J.A.Evans Shell Model and IBM Descriptions of Mixed Symmetry or Isovector M1 Transitions in the Titanium Isotopes NUCLEAR STRUCTURE 44,46,48Ti, 48Cr; calculated levels, B(M1). Shell, interacting boson models.
doi: 10.1088/0305-4616/14/2/014
1988EV01 Nucl.Phys. A489, 269 (1988) J.A.Evans, P.Van Isacker, J.P.Elliott A Test of the Interacting Boson-Fermion Model in a Single j-Shell of Neutrons and Protons NUCLEAR STRUCTURE 45Ti, 45Sc, 47V; calculated levels. Shell model.
doi: 10.1016/0375-9474(88)90153-4
1987TH05 Phys.Lett. 195B, 511 (1987) M.J.Thompson, J.P.Elliott, J.A.Evans A Microscopically Determined IBM 3 Hamiltonian NUCLEAR STRUCTURE 46Ti; calculated T = 1 spectrum. Interacting boson model.
doi: 10.1016/0370-2693(87)91563-2
1986AV03 Phys.Rev. C34, 666 (1986) F.T.Avignone III, R.L.Brodzinski, J.C.Evans, Jr., W.K.Hensley, H.S.Miley, J.H.Reeves Search for the Double-β Decay of 76Ge NUCLEAR STRUCTURE 76Ge(2β); measured neutrinoless, two-neutrino double β-decay T1/2 lower limit; deduced composite, Majorona neutrino masses.
doi: 10.1103/PhysRevC.34.666
1985AV02 Phys.Rev.Lett. 54, 2309 (1985) F.T.Avignone III, R.L.Brodzinski, D.P.Brown, J.C.Evans, Jr., W.K.Hensley, H.S.Miley, J.H.Reeves, N.A.Wogman Ultralow-Background Study of Neutrinoless Double β Decay of 76Ge: New limit on the Majorana mass of ν(e) RADIOACTIVITY 76Ge(2β-); measured neutrinoless β-decay T1/2 lower limit; deduced ν(e) Majorana mass limit. Shell model. Ultralow background Ge spectrometer.
doi: 10.1103/PhysRevLett.54.2309
1985EL12 Nucl.Phys. A437, 208 (1985) J.P.Elliott, J.A.Evans, E.E.Maqueda α-Transfer and a Tetrahedral Shape for 16O NUCLEAR STRUCTURE 16O; calculated density contours. Shell model, tetrahedral perturbation, α-clustering. NUCLEAR REACTIONS 12C(6Li, d), E=42 MeV; calculated σ(θ); deduced optical model parameters, reaction mechanism. 16O levels deduced σ enhancement factors, rotational band structure. Shell model, tetrahedral perturbation, α-clustering.
doi: 10.1016/0375-9474(85)90233-7
1985EV02 Nucl.Phys. A435, 317 (1985) J.A.Evans, J.P.Elliott, S.Szpikowski An IBM Analysis of a Single j-Shell of Neutrons and Protons NUCLEAR STRUCTURE 44,46Ti, 44Sc, 44Ca; calculated level energies; deduced shell model analog of U(6), U(5) boson labels.
doi: 10.1016/0375-9474(85)90467-1
1984HA14 Nucl.Phys. A417, 301 (1984) P.Halse, J.P.Elliott, J.A.Evans An Application of the Interacting Boson Model to the First Half of the sd Shell (1). Even-Even Nuclei NUCLEAR STRUCTURE 20,22,24Ne, 20,22O, 20,24,26,28Mg, 28Si; calculated levels, B(E2), binding energies relative to 16O. Interacting boson model.
doi: 10.1016/0375-9474(84)90510-4
1983AV01 Phys.Rev.Lett. 50, 721 (1983) F.T.Avignone III, R.L.Brodzinski, D.P.Brown, J.C.Evans, Jr., W.K.Hensley, J.H.Reeves, N.A.Wogman New Limits on the Neutrino Mass, Lepton Conservation, and No-Neutrino Double Beta Decay of 76Ge RADIOACTIVITY 76Ge; measured double β-decay T1/2 lower limit; deduced lepton conservation, neutrino mass upper limits.
doi: 10.1103/PhysRevLett.50.721
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
1979EL04 Nucl.Phys. A324, 12 (1979) The Use of an Angular Momentum Constraint in Calculating Rotational Spectra NUCLEAR STRUCTURE 8Be, 20Ne; calculated spectra. Hartree-Fock method, constraint on square of angular momentum.
doi: 10.1016/0375-9474(79)90073-3
1978PR07 Int.J.Appl.Radiat.Isotop. 29, 517 (1978) A.Prindle, J.Evans, R.Dupzyk, R.Nagle, R.Newbury The Half Life of 239Pu RADIOACTIVITY 239Pu; measured T1/2. 235U growth, α-disintegration rate. Mass spectroscopic isotope dilution, 241Am efficiency tracer techniques.
doi: 10.1016/0020-708X(78)90009-1
1975DI04 Nucl.Phys. A244, 301 (1975) H.Dirim, J.P.Elliott, J.A.Evans The Effective Hamiltonian and Spectra of the 0π Shell NUCLEAR STRUCTURE 6,7Li, 10B, 14N; calculated levels. Modified Sussex matrix elements.
doi: 10.1016/0375-9474(75)90060-3
1972EV01 Phys.Rev. C6, 1372 (1972) J.L.Evans, J.R.Cooper, D.M.Moore, W.L.Alford Positron Branching in the Decay of 143Sm, 141Nd, and 140Pr RADIOACTIVITY 143Sm, 141Nd, 140Pr; measured I(K X-ray)/Iγ ratios; deduced K/β+ ratios.
doi: 10.1103/PhysRevC.6.1372
1971BL12 Phys.Lett. 36B, 202 (1971) R.J.Blin-Stoyle, J.A.Evans, A.M.Khan Coulomb Effects in the A = 13, 18 Mirror β-Decays and the Second Class Current Problem RADIOACTIVITY 13O, 13B, 18Ne, 18F; calculated Coulomb effects on proportional differences in ft-values.
doi: 10.1016/0370-2693(71)90068-2
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
1971MA25 Nucl.Phys. A167, 16 (1971) Fractional Parentage and the Equations-of-Motion Method in Pairing Theory NUCLEAR STRUCTURE 58Ni; calculated ground-state energy. Equations-of-motion method.
doi: 10.1016/0375-9474(71)90577-X
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
1969NA10 Nucl.Phys. A137, 689 (1969) R.A.Naumann, R.F.Petry, J.S.Evans Decay of 188Au and 190Au RADIOACTIVITY 188,190Au[from spallation of Pb]; measured Eγ, Iγ, γγ-coin., ceγ-coin. 188,190Pt deduced levels. 190Hg; measured T1/2.
doi: 10.1016/0375-9474(69)90102-X
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.
1968HO17 Phys.Rev. 171, 1290 (1968) P.K.Hopke, J.S.Evans, R.A.Naumann Decay of Ho163 RADIOACTIVITY 163Ho; measured T1/2, M/L EC ratio; deduced Qβ.
doi: 10.1103/PhysRev.171.1290
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.
1968PE13 Phys.Rev. 174, 1441 (1968) R.F.Petry, R.A.Naumann, J.S.Evans Levels in Even-Even Hg192, Hg194, Hg196, and Hg198 RADIOACTIVITY 192,194,196,198Tl; measured Eγ, Iγ, I(ce), ceγ-, γγ-coin, T1/2. 192,194,196,198Hg deduced levels, J, π, ICC, γ-multipolarity, γ-mixing.
doi: 10.1103/PhysRev.174.1441
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
1967NA02 Nucl.Phys. A94, 151(1967) R.A.Naumann, R.F.Petry, J.S.Evans The Half-Life and Decay of 189Au RADIOACTIVITY 189Hg [from spallation of Pb]; measured T1/2. 189Au, measured T1/2, Eγ, Iγ. 189Pt deduced levels.
doi: 10.1016/0375-9474(67)90815-9
1967NA14 Ark.Fys. 36, 177 (1967) R.A.Naumann, R.F.Petry, J.S.Evans Nuclear Spectroscopy of Light Platinum and Mercury Isotopes NUCLEAR STRUCTURE 196Tl, 198Tl, 194Tl, 188Au, 192Tl; measured not abstracted; deduced nuclear properties.
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
1966JA12 Phys.Rev. 151, 956 (1966) A.D.Jackson, Jr., J.S.Evans, R.A.Naumann, J.D.McCullen Decay of Ag103 NUCLEAR STRUCTURE 103Ag; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.151.956
1966NA01 Bull.Am.Phys.Soc. 11, No.3, 408, KB5 (1966); and Oral Report R.A.Naumann, R.F.Petry, J.S.Evans Identification and Half-Life of Au189 NUCLEAR STRUCTURE 189Au, 189Hg; measured not abstracted; deduced nuclear properties.
1966PE06 Phys.Lett. 21, 541 (1966) R.F.Petry, R.A.Neumann, J.S.Evans Negative-Parity Levels in Even-Even Hg Isotopes NUCLEAR STRUCTURE 192Tl, 194Tl, 198Tl, 196Tl; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91292-3
1965EV02 Bull.Am.Phys.Soc. 10, No.1, 81, GC3 (1965) Decay of Pd100 NUCLEAR STRUCTURE 100Pd; measured not abstracted; deduced nuclear properties.
1965EV04 Phys.Rev. 138, B9 (1965) J.S.Evans, E.Kashy, R.A.Naumann, R.F.Petry Levels in Rh101 Populated by the Decay of Pd101 NUCLEAR STRUCTURE 101Pd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.138.B9
1965EV05 Phys.Rev. 138, B1017 (1965); Erratum Phys.Rev. 139, AB4 (1965) Decay of Pd100 to Odd-Odd Rh100 NUCLEAR STRUCTURE 100Pd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.138.B1017
1965EV06 Phys.Rev. 140, B559 (1965) Decay of Rh101m and Rh101g NUCLEAR STRUCTURE 101Rh; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B559
1965MA34 Phys.Rev. 140, B264 (1965) E.Matthias, D.A.Shirley, J.S.Evans, R.A.Naumann Half-Life and g Factor of the 75-keV Level of Rh100 NUCLEAR STRUCTURE 100Rh, 100Pd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B264
1965PE02 Bull.Am.Phys.Soc. 10, No.1, 82, GC4 (1965) R.F.Petry, J.S.Evans, E.Kashy, R.A.Naumann Levels in Rh101 Populated by the Decay of Pd101 NUCLEAR STRUCTURE 101Pd; measured not abstracted; deduced nuclear properties.
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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