NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = J.Weil Found 76 matches. 2018ST17 Phys.Rev. C 98, 054908 (2018) J.Staudenmaier, J.Weil, V.Steinberg, S.Endres, H.Petersen Dilepton production and resonance properties within a new hadronic transport approach in the context of the GSI-HADES experimental data
doi: 10.1103/PhysRevC.98.054908
2018ZH12 Phys.Rev. C 97, 034625 (2018) Y.-X.Zhang, Y.-J.Wang, M.Colonna, P.Danielewicz, A.Ono, M.B.Tsang, H.Wolter, J.Xu, L.-W.Chen, D.Cozma, Z.-Q.Feng, S.Das Gupta, N.Ikeno, C.-M.Ko, B.-A.Li, Q.-F.Li, Z.-X.Li, S.Mallik, Y.Nara, T.Ogawa, A.Ohnishi, D.Oliinychenko, M.Papa, H.Petersen, J.Su, T.Song, J.Weil, N.Wang, F.g-S.Zhang, Z.Zhang Comparison of heavy-ion transport simulations: Collision integral in a box
doi: 10.1103/PhysRevC.97.034625
2016GA35 Phys.Rev. C 94, 035502 (2016) K.Gallmeister, U.Mosel, J.Weil Neutrino-induced reactions on nuclei NUCLEAR REACTIONS 12C(e, e'), E=240, 560 MeV; calculated inclusive σ(E, θ). 12C(ν, μ), (ν-bar, μ), at Q2<1 GeV2; calculated double differential cross sections and forward angle double differential cross section per neutron and per proton using Giessen-Boltzmann-Uehling-Uhlenbeck (GiBUU) quantum-kinetic transport theory with improvements in the treatment of nuclear g.s. and 2p2h interactions. Comparison with experimental data from MiniBooNE collaboration.
doi: 10.1103/PhysRevC.94.035502
2016MA04 Phys.Rev. C 93, 014301 (2016) R.Massarczyk, G.Schramm, T.Belgya, R.Schwengner, R.Beyer, D.Bemmerer, Z.Elekes, E.Grosse, R.Hannaske, A.R.Junghans, Z.Kis, T.Kogler, C.Lorenz, K.Schmidt, L.Szentmiklosi, A.Wagner, J.L.Weil Role of electric and magnetic dipole strength functions in the 114Cd (γ, γ') and 113Cd (n, γ) reactions NUCLEAR REACTIONS 114Cd(γ, γ'), E<10 MeV; measured Eγ, Iγ, γ(θ), photoabsorption σ(E) at bremsstrahlung facility γELBE at Dresden. 113Cd(n, γ), E=cold neutrons; measured Eγ, Iγ at Budapest reactor facility; deduced electric and magnetic dipole γ-strength function below S(n). Triple Lorentzian model (TLO). Comparison with statistical model calculations using γDEX code using RIPL3 M1 and triple Gaussian models.
doi: 10.1103/PhysRevC.93.014301
2016WE14 Phys.Rev. C 94, 054905 (2016) J.Weil, V.Steinberg, J.Staudenmaier, L.G.Pang, D.Oliinychenko, J.Mohs, M.Kretz, T.Kehrenberg, A.Goldschmidt, B.Bauchle, J.Auvinen, M.Attems, H.Petersen Particle production and equilibrium properties within a new hadron transport approach for heavy-ion collisions
doi: 10.1103/PhysRevC.94.054905
2016XU03 Phys.Rev. C 93, 044609 (2016) J.Xu, L.-W.Chen, M.Y.B.Tsang, H.Wolter, Y.-X.Zhang, J.Aichelin, M.Colonna, D.Cozma, P.Danielewicz, Z.-Q.Feng, A.Le Fevre, T.Gaitanos, C.Hartnack, K.Kim, Y.Kim, C.-M.Ko, B.-A.Li, Q.-F.Li, Z.-X.Li, P.Napolitani, A.Ono, M.Papa, T.Song, J.Su, J.-L.Tian, N.Wang, Y.-J.Wang, J.Weil, W.-J.Xie, F.-S.Zhang, G.-Q.Zhang Understanding transport simulations of heavy-ion collisions at 100A and 400A MeV: Comparison of heavy-ion transport codes under controlled conditions
doi: 10.1103/PhysRevC.93.044609
2015EN03 Phys.Rev. C 91, 054911 (2015) S.Endres, H.van Hees, J.Weil, M.Bleicher Coarse-graining approach for dilepton production at energies available at the CERN Super Proton Synchrotron
doi: 10.1103/PhysRevC.91.054911
2015EN04 Phys.Rev. C 92, 014911 (2015) S.Endres, H.van Hees, J.Weil, M.Bleicher Dilepton production and reaction dynamics in heavy-ion collisions at SIS energies from coarse-grained transport simulations
doi: 10.1103/PhysRevC.92.014911
2013MA32 Phys.Rev. C 87, 044306 (2013) R.Massarczyk, G.Schramm, A.R.Junghans, R.Schwengner, M.Anders, T.Belgya, R.Beyer, E.Birgersson, A.Ferrari, E.Grosse, R.Hannaske, Z.Kis, T.Kogler, K.Kosev, M.Marta, L.Szentmiklosi, A.Wagner, J.L.Weil Electromagnetic dipole strength up to the neutron separation energy from 196Pt(γγ')and 195Pt(n, γ) reactions NUCLEAR REACTIONS 195Pt(n, γ), E(mean)=12 meV; measured Eγ, Iγ at the research reactor in Budapest. 196Pt(γ, γ'), E=0-7.9 MeV; measured Eγ, Iγ, bremsstrahlung photon fluences, photoabsorption σ(E) at the ELBE accelerator in Dresden; deduced E1 and M1 strength distributions, simulated ground-state branching ratios for 1- states. Analysis by statistical code γDEX.
doi: 10.1103/PhysRevC.87.044306
2013TH10 Eur.Phys.J. A 49, 132 (2013) M.Thiel, V.Metag, P.Aguar-Bartolome, L.K.Akasoy, J.R.M.Annand, H.J.Arends, K.Bantawa, R.Beck, V.Bekrenev, H.Berghauser, A.Braghieri, W.J.Briscoe, J.Brudvik, S.Cherepnya, M.Dieterle, E.J.Downie, P.Drexler, L.V.Filkov, S.Friedrich, D.I.Glazier, R.Gregor, E.Heid, D.Hornidge, O.Jahn, T.C.Jude, V.L.Kashevarov, I.Keshelashvili, R.Kondratiev, M.Korolija, M.Kotulla, B.Krusche, A.Kulbardis, B.Lemmer, V.Lisin, K.Livingston, S.Lugert, I.J.D.MacGregor, Y.Maghrbi, J.Mancell, D.M.Manley, M.Martinez, J.C.McGeorge, E.F.McNicoll, D.G.Middleton, A.Mushkarenkov, M.Nanova, B.M.K.Nefkens, A.Nikolaev, R.W.Novotny, M.Ostrick, P.Pedroni, F.Pheron, A.Polonski, S.N.Prakhov, J.Robinson, G.Rosner, T.Rostomyan, S.Schumann, M.H.Sikora, A.Starostin, I.Supek, A.Thomas, M.Unverzagt, D.P.Watts, J.Weil, D.Werthmuller, I.Zamboni In-medium modifications of the ω meson near the production threshold
doi: 10.1140/epja/i2013-13132-6
2012SC02 Phys.Rev. C 85, 014311 (2012) G.Schramm, R.Massarczyk, A.R.Junghans, T.Belgya, R.Beyer, E.Birgersson, E.Grosse, M.Kempe, Z.Kis, K.Kosev, M.Krticka, A.Matic, K.D.Schilling, R.Schwengner, L.Szentmiklosi, A.Wagner, J.L.Weil Dipole strength in 78Se below the neutron separation energy from a combined analysis of 77Se(n, γ) and 78Se(γ, γ') experiments NUCLEAR REACTIONS 77Se(n, γ), E AP 6 milli-eV, cold neutrons; 78Se(γ, γ'), E<11.5 MeV bremsstrahlung; measured Eγ, Iγ; deduced photoabsorption cross section, level density according to constant-temperature model, dipole strength function. Comparison with simulated spectra from extreme statistical code.
doi: 10.1103/PhysRevC.85.014311
2012WE12 Eur.Phys.J. A 48, 111 (2012); Erratum Eur.Phys.J. A 48, 150 (2012) Dilepton production in proton-induced reactions at SIS energies with the GiBUU transport model
doi: 10.1140/epja/i2012-12111-9
2006AS02 Phys.Rev. C 73, 055801 (2006) M.Assuncao, M.Fey, A.Lefebvre-Schuhl, J.Kiener, V.Tatischeff, J.W.Hammer, C.Beck, C.Boukari-Pelissie, A.Coc, J.J.Correia, S.Courtin, F.Fleurot, E.Galanopoulos, C.Grama, F.Haas, F.Hammache, F.Hannachi, S.Harissopulos, A.Korichi, R.Kunz, D.LeDu, A.Lopez-Martens, D.Malcherek, R.Meunier, Th.Paradellis, M.Rousseau, N.Rowley, G.Staudt, S.Szilner, J.P.Thibaud, J.L.Weil E1 and E2 S factors of 12C(α, γ0)160 from γ-ray angular distributions with a 4π-detector array NUCLEAR REACTIONS 12C(α, γ), E(cm)=1.30-2.78 MeV; measured Eγ, Iγ(θ); deduced E1 and E2 astrophysical S-factors.
doi: 10.1103/PhysRevC.73.055801
2005BA02 Nucl.Phys. A747, 206 (2005) D.Bandyopadhyay, N.Warr, C.Fransen, N.Boukharouba, V.Werner, S.W.Yates, J.L.Weil, M.T.McEllistrem Three-phonon excitations in 124Sn NUCLEAR REACTIONS 124Sn(n, n'γ), E=2.2-4.5 MeV; measured Eγ, Iγ, γγ-coin, excitation functions, angular distributions, DSA. 124Sn deduced levels, J, π, T1/2, two- and three-phonon excitations.
doi: 10.1016/j.nuclphysa.2004.10.003
2005HA16 Nucl.Phys. A752, 514c (2005) J.W.Hammer, M.Fey, R.Kunz, J.Kiener, V.Tatischeff, F.Haas, J.L.Weil, M.Assuncao, C.Beck, C.Boukari-Pelissie, A.Coc, J.J.Correia, S.Courtin, F.Fleurot, E.Galanopoulos, C.Grama, F.Hammache, S.Harissopulos, A.Korichi, E.Krmpotic, D.Le Du, A.Lopez-Martens, D.Malcherek, R.Meunier, P.Papka, T.Paradellis, M.Rousseau, N.Rowley, G.Staudt, S.Szilner New determination of the 12C(α, γ)16O reaction rate from γ-ray angular distribution measurements NUCLEAR REACTIONS 12C(α, γ), E(cm)=0.89-2.8 MeV; measured σ(θ), S-factors; deduced astrophysical reaction rate.
doi: 10.1016/j.nuclphysa.2005.02.056
2005HA48 Nucl.Phys. A758, 363c (2005) J.W.Hammer, M.Fey, R.Kunz, J.Kiener, V.Tatischeff, F.Haas, J.L.Weil, M.Assuncao, C.Beck, C.Boukari-Pelissie, A.Coc, J.J.Correia, S.Courtin, F.Fleurot, E.Galanopoulos, C.Grama, F.Hammache, S.Harissopulos, A.Korichi, E.Krmpotic, D.Le Du, A.Lopez-Martens, D.Malcherek, R.Meunier, P.Papka, T.Paradellis, M.Rousseau, N.Rowley, G.Staudt, S.Szilner E1 and E2 capture cross section and astrophysical reaction rate of the key reaction 12C(α, γ)16O NUCLEAR REACTIONS 12C(α, γ), E(cm)=0.89-2.8 MeV; measured Eγ, Iγ, angular distributions; deduced S-factors for E1 and E2 capture. Eurogam and Gandi arrays, astrophysical implications discussed.
doi: 10.1016/j.nuclphysa.2005.05.066
2001CH03 Phys.Rev. C63, 014606 (2001) G.Chen, M.Li, J.L.Weil, M.T.McEllistrem Neutron Scattering in 140, 142Ce and Strengths of Neutrons and Protons in Collective Levels of 140Ce NUCLEAR REACTIONS 140,142Ce(n, n), (n, n'), E=7.5 MeV; measured σ(θ). 140,142Ce deduced level configurations. Comparisons with model predictions.
doi: 10.1103/PhysRevC.63.014606
2001GA55 Phys.Rev. C64, 047303 (2001) Z.Gacsi, M.Csatlos, A.Krasznahorkay, D.Sohler, J.Gulyas, J.Timar, M.Hunyadi, J.L.Weil, J.van Klinken Low-Lying, Excited K = 0 Bands in 238U NUCLEAR REACTIONS 234,236,238U(α, α'), E=19 MeV; measured Eγ, Iγ, E(ce), I(ce) following Coulomb excitation. 238U deduced transitions ICC, enhancement of E0 strength, K=0 bands moments of inertia.
doi: 10.1103/PhysRevC.64.047303
2001MA74 Int.J.Mod.Phys. E10, 209 (2001) A.Marinov, S.Gelberg, D.Kolb, J.L.Weil Strongly Enhanced Low Energy α-Particle Decay in Heavy Actinide Nuclei and Long-Lived Superdeformed and Hyperdeformed Isomeric States NUCLEAR REACTIONS W(p, X), E=24 GeV; measured delayed Eα; deduced possible isomeric origin. 236Am, 236,238Bk, 247Es, 252No deduced yields from secondary fusion reactions. RADIOACTIVITY 238mAm, 247mEs, 252mNo(α); measured isomer decay Eα, T1/2; deduced possible transitions between hyperdeformed and superdeformed states.
doi: 10.1142/S0218301301000472
1993IG01 Phys.Rev. C47, 1504 (1993) A.V.Ignatyuk, J.L.Weil, S.Raman, S.Kahane Density of Discrete Levels in 116Sn NUCLEAR STRUCTURE 116Sn; analyzed level data; deduced best model fit to discrete level density. Back-shifted Fermi gas, constant temperature, generalized superfluid model.
doi: 10.1103/PhysRevC.47.1504
1991BE26 Appl.Radiat.Isot. 42, 683 (1991) R.K.Bera, J.L.Weil, S.W.Yates, M.Jay Production of [11C] Carbon Dioxide via the 11B(p, n)11C Reaction and [18F] Fluoride via the 18O(p, n)18F Reaction for Radiopharmaceutical Development
doi: 10.1016/0883-2889(91)90040-8
1991RA01 Phys.Rev. C43, 521 (1991) S.Raman, T.A.Walkiewicz, S.Kahane, E.T.Jurney, J.Sa, Z.Gacsi, J.L.Weil, K.Allaart, G.Bonsignori, J.F.Shriner, Jr. Nearly Complete Level Scheme of 116Sn Below 4.3 MeV NUCLEAR REACTIONS 115Sn(n, γ), E=thermal; 116Sn(n, n'γ), E ≤ 4.5 MeV; measured Eγ, Iγ, γ(θ) vs E. 116Sn deduced levels, J, π, neutron separation energy.
doi: 10.1103/PhysRevC.43.521
1989HI11 Phys.Rev. C40, 2509 (1989) S.E.Hicks, Z.Cao, M.C.Mirzaa, J.L.Weil, J.M.Hanly, J.Sa, M.T.McEllistrem Nuclear Dynamics of 192Os as Probed in Neutron Scattering NUCLEAR REACTIONS 192Os(n, n), (n, n'), E=0.25-4.2 MeV; measured σ(θ), σ(E); deduced model parameters. 192Os deduced deformation features. Coupled-channels analysis.
doi: 10.1103/PhysRevC.40.2509
1989KO29 Phys.Rev. C40, R1093 (1989) M.A.Kovash, B.Anderson-Pugh, M.T.McEllistrem, J.K.Ternes, J.H.Trice, J.L.Weil, S.L.Blatt, H.J.Hausman, D.G.Marchlenski, A.D.Bacher Quadrupole and Octupole Radiation from 16O Near 39 MeV Excitation NUCLEAR REACTIONS 15N(polarized p, γ), E=24.4, 28.8 MeV; measured Eγ, Iγ, σ(θ), analyzing power vs θ; deduced σ(E2)/σ(E1), σ(E3)/σ(E1). 16O deduced isovector quadrupole, octupole resonance components.
doi: 10.1103/PhysRevC.40.R1093
1985LE10 Phys.Rev. C32, 277 (1985) R.S.Lee, J.H.Hamilton, A.V.Ramayya, A.P.de Lima, D.L.Sastry, K.S.R.Sastry, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.-D.Schmidt-Ott, J.Lin, C.R.Bingham, L.L.Riedinger, E.F.Zganjar, J.L.Weil, B.D.Kern, A.C.Xenoulis, R.W.Fink, Sun Xi-jun, Guo Jun-sheng, Cho Chi-cheng, Pan Zong-you, Guo Ying-xian Decay of 117Xe → 117I → 117Te NUCLEAR REACTIONS 107,109Ag(12C, xn), E=50-70 MeV; measured γ yields. 117I deduced transition. RADIOACTIVITY 117Xe(EC), (β+) [from 104Pd(16O, xn), E=86 MeV]; 117I(EC), (β+) [from 117Xe β-decay]; 117Te(β+), (EC) [from 117I β-decay]; measured Eγ, Iγ, E X-ray, I X-ray, T1/2, γγ-coin. 117I, 117Te deduced levels, relative Iγ. 117Sb(EC), (β+) [from 117Te decay]; measured T1/2. 117Xe, 117I deduced mass difference, Q(EC).
doi: 10.1103/PhysRevC.32.277
1985MI20 Phys.Rev. C32, 1488 (1985) M.C.Mirzaa, J.P.Delaroche, J.L.Weil, J.Hanly, M.T.McEllistrem, S.W.Yates Collective Excitations of 194Pt in Low Energy Neutron Scattering NUCLEAR REACTIONS 194Pt(n, n), (n, n'), E=2.5 MeV; measured σ(θ); deduced potential parameters. Pt(n, n), E=1-20 MeV; analyzed σ(E). 194Pt deduced shape characteristics. Coupled-channels calculation.
doi: 10.1103/PhysRevC.32.1488
1984BE05 Phys.Rev. C29, 709 (1984) R.E.Benenson, M.T.McEllistrem, J.L.Weil, W.R.Coker, T.Tamura Interference between Reaction Mechanisms in 32S(3He, n)34Ar NUCLEAR REACTIONS 32S(3He, n), E=4.6-6.5 MeV; measured σ(θ) vs E; deduced optical model parameters. 35Ar deduced resonances, J, π, Γ, partial widths. Direct, compound reaction interference effects, DWBA. Tof.
doi: 10.1103/PhysRevC.29.709
1984HA44 Phys.Rev. C30, 1454 (1984) R.W.Harper, J.L.Weil, J.D.Brandenberger Interaction of Neutrons with Even-A Tin Isotopes: Neutron-excess dependence in scattering at E(n) = 1.00 and 1.63 MeV NUCLEAR REACTIONS 116,118,120,122,124Sn(n, n), (n, n'), E=1, 1.63 MeV; measured σ(θ); deduced optical model parameters, neutron excess parameter dependence. Isotopically enriched samples, neutron tof. Compound-elastic scattering, level width fluctuation corrections.
doi: 10.1103/PhysRevC.30.1454
1984KE09 ATOMKI Kozlem. 26, 26 (1984) B.D.Kern, M.T.McEllistrem, J.L.Weil, S.W.Yates Nuclear Structure Studies through the Combined Use of the (n, n') and (n, n'γ) Reactions NUCLEAR REACTIONS 94,100Mo, 124Sn, 168Er, 198Pt(n, n'), (n, n'γ), E=0.5-4 MeV; measured σ(E), σ(E, Eγ), σ(θn), γ(θ). 94,100Mo, 198Pt levels deduced J.
1983YA04 Nucl.Phys. A406, 519 (1983) S.W.Yates, A.Khan, A.J.Filo, M.C.Mirzaa, J.L.Weil, M.T.McEllistrem Low-Lying Levels, γ-Ray Transitions, and Vibrational Structure in 198Pt from (n, n'γ) Reaction Spectroscopy NUCLEAR REACTIONS 198Pt(n, n'γ), E=0.8-2.5 MeV; measured Eγ, Iγ, σ(E, Eγ, θγ). 198Pt deduced levels, J, π, branching ratios. Enriched target, Ge(Li) detector, time-of-flight background suppression. Theoretical comparison.
doi: 10.1016/0375-9474(83)90374-3
1982HA47 Phys.Rev. C26, 1432 (1982) R.W.Harper, T.W.Godfrey, J.L.Weil Interaction of Neutrons with Even-A Tin Isotopes. I. Total Cross Section for E(n) = 0.3-5.0 MeV NUCLEAR REACTIONS 116,118,120,122,124Sn(n, X), E=0.3-5 MeV; measured transmission; deduced σ(total) vs E. Tof, enriched targets. Optical model.
doi: 10.1103/PhysRevC.26.1432
1981FI01 Phys.Rev. C23, 1938 (1981) A.J.Filo, S.W.Yates, D.F.Coope, J.L.Weil, M.T.McEllistrem Positive-and Negative-Parity Level Structures of 194Pt from (n, n'γ) Reaction Spectroscopy NUCLEAR REACTIONS 194Pt(n, n'), E=1.2-4.5 MeV; measured Eγ, Iγ, σ(E, Eγ), γ(θ). 194Pt deduced levels, γ-branching ratios, J, π, B(E2). Enriched target, Ge(Li) detector. Interacting boson, boson expansion models.
doi: 10.1103/PhysRevC.23.1938
1978FL07 Phys.Rev. C18, 1566 (1978) D.S.Flynn, K.K.Sekharan, B.A.Hiller, H.Laumer, J.L.Weil, F.Gabbard Cross Sections and Reaction Rates for 23Na(p, n)23Mg, 27Al(p, n)27Si, 27Al(α, n)30P, 29Si(α, n)32S, and 30Si(α, n)33S NUCLEAR REACTIONS 23Na, 27Al(p, n), E=5.0-6.5 MeV; 27Al, 29,30Si(α, n), E=2.8-6.8 MeV; measured σ(E). 27Si(n, p), E=0-0.55 MeV; 30P(n, α), E=0.4-0.9 MeV; 32,33S(n, α), E=0-2.3 MeV; deduced σ(E); deduced nucleosynthesis reaction rates. 23Mg(n, p), E=0-3 MeV; calculated σ(E); deduced nucleosynthesis reaction rates.
doi: 10.1103/PhysRevC.18.1566
1978GL04 Phys.Rev. C18, 2520 (1978) G.P.Glasgow, F.D.McDaniel, J.L.Weil, J.D.Brandenberger, M.T.McEllistrem Level and Decay Scheme Studies in 92Zr and 94Zr via (n, n'γ) Reactions NUCLEAR REACTIONS 92,94Zr(n, n'γ), E=2.2-3.7 MeV; measured Eγ, σ(E, Eγ, 90°), σ(Eγ, θγ). 92,94Zr deduced levels, δ, J, π, branching ratio. Enriched targets, Ge(Li) detectors, tof background suppression. Statistical model calculation.
doi: 10.1103/PhysRevC.18.2520
1977CO26 Phys.Rev. C16, 2223 (1977) D.F.Coope, S.N.Tripathi, M.C.Schell, J.L.Weil, M.T.McEllistrem Strong Collective Excitations in Low Energy Neutron Scattering from Transitional Nuclei NUCLEAR REACTIONS 148,150,152Sm(n, n), (n, n'), (n, n'γ), E=2.47 MeV; measured σ(θ). Coupled channels, statistical model analysis.
doi: 10.1103/PhysRevC.16.2223
1976BI09 Phys.Rev. C14, 1586 (1976) C.R.Bingham, L.L.Riedinger, F.E.Turner, B.D.Kern, J.L.Weil, K.J.Hofstetter, J.Lin, E.F.Zganjar, A.V.Ramayya, J.H.Hamilton, J.L.Wood, G.M.Gowdy, R.W.Fink, E.H.Spejewski, W.D.Schmidt-Ott, R.L.Mlekodaj, H.K.Carter, K.S.R.Sastry Decay of Mass-Separated 190Tl and 190Hg RADIOACTIVITY 190,190mTl, 190Hg [from Ta, W(16O, X)]; measured Eγ, Iγ, I(ce), Eβ, γX-ray-coin, γγ-coin, T1/2; deduced log ft, Q, ICC. 190Hg, 190Au deduced levels, J, π, λ.
doi: 10.1103/PhysRevC.14.1586
1976GO02 Phys.Rev. C13, 1601 (1976) G.M.Gowdy, A.C.Xenoulis, J.L.Wood, K.R.Baker, R.W.Fink, J.L.Weil, B.D.Kern, K.J.Hofstetter, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.D.Schmidt-Ott, J.Lin, C.R.Bingham, L.L.Riedinger, E.F.Zganjar, K.S.R.Sastry, A.V.Ramayya, J.H.Hamilton On-Line Mass Separator Investigation of the New Isotope 2.9-sec 116I RADIOACTIVITY 116I, 116Xe; measured Eγ, Iγ, T1/2, βγ(t); deduced Q, log ft. 116I deduced J, π. 116Te, 116Xe deduced levels, J, π.
doi: 10.1103/PhysRevC.13.1601
1976HA25 Izv.Akad.Nauk SSSR, Ser.Fiz. 40, 2 (1976); Bull.Acad.Sci.USSR, Phys.Ser. 40, No.1, 1 (1976) J.H.Hamilton, K.R.Baker, C.R.Bingham, E.L.Bosworth, H.K.Carter, J.D.Cole, R.W.Fink, G.Garcia Bermudez, G.W.Gowdy, K.J.Hofstetter, M.A.Ijaz, A.C.Kahler, B.D.Kern, W.Lourens, B.Martin, R.L.Mlekodaj, A.V.Ramayya, L.L.Riedinger, W.D.Schmidt-Ott, E.H.Spejewski, B.N.Subba Rao, E.L.Robinson, K.S.Toth, F.Turner, J.L.Weil, J.L.Wood, A.Xenoulis, E.F.Zganjar New Isotope 193Pb and the Structure of 193Tl; Shape Coexistence in 188Hg and in 189Au; and a New Ion Source: Recent UNISOR Research RADIOACTIVITY 193Pb; measured T1/2, Eγ, Iγ, γγ-coin. 188Tl; measured Eγ, Iγ, γγ-coin, I(ce), γce-coin. 189Tl, 189Hg; measured Eγ, Iγ, γγ-, γX-, γce-coin. 188,189Hg, 193Tl deduced levels, J, π, shape isomers.
1975HA27 Phys.Rev.Lett. 35, 562 (1975) J.H.Hamilton, A.V.Ramayya, E.L.Bosworth, W.Lourens, J.D.Cole, B.Van Nooijen, G.Garcia-Bermudez, B.Martin, B.N.Subba Rao, H.Kawakami, L.L.Riedinger, C.R.Bingham, F.Turner, E.F.Zganjar, E.H.Spejewski, H.K.Carter, R.L.Mlekodaj, W.D.Schmidt-Ott, K.R.Baker, R.W.Fink, G.M.Gowdy, J.L.Wood, A.Xenoulis, B.D.Kern, K.J.Hofstetter, J.L.Weil, K.S.Toth, M.A.Ijaz, K.F.R.Faftry Crossing of Near-Spherical and Deformed Bands in 186,188Hg and New Isotopes 186,188Tl RADIOACTIVITY 186,188Tl [from 181Ta(16O, 9nγ), (16O, 11nγ), E=143-145 MeV]; measured T1/2, Eγ, Iγ, γce-, γγ-coin, γ(t); deduced ICC. 186,188Hg deduced levels, J, π, K.
doi: 10.1103/PhysRevLett.35.562
1975ZG01 Phys.Lett. 58B, 159 (1975) E.F.Zganjar, J.L.Wood, R.W.Fink, L.L.Riedinger, C.R.Bingham, B.D.Kern, J.L.Weil, J.H.Hamilton, A.V.Ramayya, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.D.Schmidt-Ott Rotation-Aligned Coupling and Axial Asymmetry in 189-195Au RADIOACTIVITY 189,189m,191,191m,193Hg; measured γγ(t), γ X-ray(t), Eγ, Iγ, I(ce); deduced ICC. 189,191,193Au deduced levels. 189,191,193,195Au deduced systematics.
doi: 10.1016/0370-2693(75)90627-9
1974HA10 Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2036 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 22 (1974) J.H.Hamilton, E.H.Spejewski, R.L.Mlekodaj, W.-D.Schmidt-Ott, R.W.Fink, A.Xenoulis, K.R.Baker, J.L.Wood, G.Gowdy, H.K.Carter, B.D.Kern, K.J.Hofstetter, J.L.Weil, E.F.Zganjar, K.S.R.Sastry, F.T.Avignone, C.R.Bingham, L.L.Riedinger, L.Harwood, F.Turner, I.A.Sellin, D.J.Pegg, J.Lin, A.V.Ramayya, S.Lee, G.Garcia-Bermudez, E.Bosworth, K.S.Toth, N.R.Johnson Initial UNISOR Research: New Isotopes 186Tl, 188Tl, 116I; Decays of 189,190Tl, 117Xe, and 117I; and Off-Line Atomic and Nuclear Studies RADIOACTIVITY 116,117Xe, 116,117I, 186,188,189,190Tl; measured T1/2, Eγ, Iγ, γγ, Eβ; deduced Q(β). 126I measured γγ(θ, H). 117I, 116Te, 188,190Hg deduced levels, J, π. 126Xe level deduced g. On-line isotope separator UNISOR.
1973GL03 Priv.Comm. (June 1973) G.P.Glasgow, F.D.McDaniel, L.D.Brandenburger, J.L.Weil, M.T.McEllistrem Resolution of Ambiguities in the Level Scheme of 94Zr
1973OB02 Phys.Rev. C7, 1076 (1973) Scattering of 9.8-MeV Neutrons from Silicon and Sulfur NUCLEAR REACTIONS Si, S(n, n'), E=9.8 MeV; measured σ(En', θ). Deduced optical model parameters.
doi: 10.1103/PhysRevC.7.1076
1972AL45 Phys.Lett. 41B, 577 (1972) B.W.Allardyce, C.J.Batty, D.J.Baugh, E.Friedman, G.Heymann, J.L.Weil, M.E.Cage, G.J.Pyle, G.T.A.Squier, A.S.Clough, J.Cox, D.F.Jackson, S.Murugesu, V.Rajaratnam Ratio of Pion-Nucleus Reaction Cross Sections and the Neutron Density Distribution for Lead NUCLEAR REACTIONS C, Pb(π-, X), (π+, X), E=0.71-2.0 GeV/c; measured σ ratios.
doi: 10.1016/0370-2693(72)90638-7
1972GA13 Phys.Rev. C5, 1508 (1972) W.Galati, J.D.Brandenberger, J.L.Weil Scattering of Neutrons by Carbon from 3 to 7 MeV NUCLEAR REACTIONS C(n, n), (n, n'), E=3-7 MeV; measured σ(E;θ); deduced phase shifts. 13C resonances deduced J, π, level-width.
doi: 10.1103/PhysRevC.5.1508
1972OB01 Phys.Rev. C5, 738 (1972) A.W.Obst, T.B.Grandy, J.L.Weil Reaction 9Be(α, n)12C from 1.7 to 6.4 MeV NUCLEAR REACTIONS 9Be(α, n), E=1.69-6.44 MeV; measured σ(E;θ).
doi: 10.1103/PhysRevC.5.738
1972SC28 Nucl.Phys. A192, 609 (1972) R.L.Schulte, M.Cosack, A.W.Obst, J.L.Weil 2H+d Reactions from 1.96 to 6.20 MeV NUCLEAR REACTIONS 2H(d, d), 2H(d, 3He), 2H(d, t), 2H(d, p), 2H(d, n), E=2.0-6.2 MeV; measured σ(E, θ); deduced 2H(d, n) σ(θ). Enriched target.
doi: 10.1016/0375-9474(72)90093-0
1971DI12 Aust.J.Phys. 24, 139 (1971) The 18O(3He, n0)20Ne and 18O(3He, n1)20Ne Reactions from 2.0 to 4.6 MeV NUCLEAR REACTIONS 18O(3He, n), E=2-4.6 MeV; measured σ(E;θ); deduced reaction mechanism.
1969CO14 Nucl. Phys. A136, 532 (1969) M.Cosack, M.K.Leung, M.T.McEllistrem, R.L.Schulte, M.M.Stautberg, J.L.Weil, J.C.Norman Threshold Effects in the 40Ar(d, p)41Ar Reaction NUCLEAR REACTIONS 40Ar(d, p), E = 2.10-5.45 MeV; measured σ(E;Ep, θ). 40Ar(d, np), E =4.2-5.0 MeV; measured σ(E;Ep, θ); deduced (d, n) threshold. Natural target.
doi: 10.1016/0375-9474(69)90125-0
1968SC11 Phys.Rev. 172, 1139 (1968) H.L.Scott, W.Galati, J.L.Weil, M.T.McEllistrem Proton-Induced Reactions on 40Ar and Analogs of 41Ar Levels NUCLEAR STRUCTURE 41K; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.172.1139
1967BA40 Phys.Rev. 161, 928 (1967) A.W.Barrows, Jr., F.Gabbard, J.L.Weil 19F(d, n)20Ne Reaction from 2.5 to 6.5 MeV NUCLEAR STRUCTURE 19F, 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.161.928
1966DI04 Nucl.Phys. 86, 509(1966) The Reactions 11B(3He, N)13N and 7Li(3He, N)9B from 1.5 to 5.5 MeV Bombarding Energy NUCLEAR REACTIONS 7Li, 11B(3He, n0), E = 1.5-5.5 MeV; measured σ(E, θ). 10B, 14N deduced levels, level-width. Enriched targets.
doi: 10.1016/0029-5582(66)90493-7
1966SW04 Nucl.Phys. 86, 119(1966) J.B.Swint, A.C.L.Barnard, T.B.Clegg, J.L.Weil Cross Sections as a Function of Energy for the Scattering of Protons from 12C NUCLEAR REACTIONS 12C(p, p), E = 4.7-12.8 MeV; 12C(p, p'), E = 6.0-12.8 MeV; measured σ(E, θ). 13N deduced levels. Natural target.
doi: 10.1016/0029-5582(66)90295-1
1965DI06 Nucl.Phys. 71, 641 (1965) The Reaction Be9(He3, n)C11 from 1.3 to 5.4 MeV NUCLEAR REACTIONS 9Be(3He, n), E = 1.30-5.35 MeV; measured σ(E;En, θ), L.
doi: 10.1016/0029-5582(65)90772-8
1965DI07 Nucl.Phys. 73, 161 (1965) The 13C(3He, n0)15O Reaction at 1.4 to 5.8 MeV NUCLEAR REACTIONS 13C(3He, n), E = 1.4-5.8 MeV; measured σ(E;θ n). Enriched target.
doi: 10.1016/0029-5582(65)90163-X
1964BA08 Nucl. Phys. 50, 604 (1964) A.C.L.Barnard, C.M.Jones, J.L.Weil Elastic Scattering of 2-11 MeV Protons by He4
doi: 10.1016/0029-5582(64)90233-0
1964BA40 Bull. Am. Phys. Soc. 9, No. 6, 665, Y3 (1964) A.Barrows, F.Gabbard, J.L.Weil, T.Young F19(d, n)Ne20 Reaction, 2.5-6.0 MeV NUCLEAR STRUCTURE 19F, 20Ne; measured not abstracted; deduced nuclear properties.
1964CL03 Nucl. Phys. 50, 621 (1964) T.B.Clegg, A.C.L.Barnard, J.B.Swint, J.L.Weil The Elastic Scattering of Protons from He3 from 4.5 to 11.5 MeV
doi: 10.1016/0029-5582(64)90234-2
1964SI09 Nucl.Phys. 52, 273 (1964) R.H.Siemssen, R.Felst, M.Cosack, J.L.Weil The Reaction F19(d, n)Ne20 NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90692-3
1964SW02 Bull.Am.Phys.Soc. 9, No.4, 408, CA11 (1964) J.B.Swint, T.B.Clegg, J.L.Weil, C.M.Jones, A.C.L.Barnard Scattering of Protons by 12C NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1963BA04 Bull.Am.Phys.Soc. 8, No.2, 124, U4 (1963) A.C.L.Barnard, C.M.Jones, J.L.Weil He4(p, p)He4 Reaction and Phase Shifts NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
1963CL01 Bull.Am.Phys.Soc. 8, No.2, 124, U3 (1963) T.B.Clegg, A.C.L.Barnard, J.B.Swint, J.L.Weil He3(p, p)He3, 4.5-10.4 MeV NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
1963DI01 Bull.Am.Phys.Soc. 8, No.2, 115, I4 (1963) Excitation Functions of Li7(He3, n)B9 and O18(He3, n)Ne20 and the Angular Distribution of O18(He3, n)Ne20 NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1963SC03 Bull.Am.Phys.Soc. 8, No.2, 127, V6 (1963) H.D.Scott, P.H.Stelson, J.L.Weil, A.C.L.Barnard Differential Cross Sections for Reactions from Protons on A40 NUCLEAR STRUCTURE 40Ar; measured not abstracted; deduced nuclear properties.
1963WE01 Bull.Am.Phys.Soc. 8, No.2, 115, I5 (1963) J.L.Weil, M.Cosack, R.Felst, R.Siemssen Angular Distributions of F19(d, n)Ne20 NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
1962TO12 Nuclear Phys. 39, 541 (1962); Erratum Nucl.Phys. 43, 528 (1963) T.A.Tombrello, C.Miller Jones, G.C.Phillips, J.L.Weil The Scattering of Protons from He3 NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90412-1
1962WE01 Bull.Am.Phys.Soc. 7, No.1, 59, R5 (1962) J.L.Weil, G.U.Din, H.M.Kuan, P.R.Almond Be9(He3, n)C11 Reaction NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1962WE03 Bull.Am.Phys.Soc. 7, No.2, 111, A5 (1962) B11(He3, n)N13 and C13(He3, n)O15 Reactions NUCLEAR STRUCTURE 11B, 13C; measured not abstracted; deduced nuclear properties.
1961TO09 Bull.Am.Phys.Soc. 6, No.6, 507, E14 (1961) T.A.Tombrello, C.M.Jones, G.C.Phillips, J.L.Weil Elastic Scattering of Protons from He3 NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
1960RE02 Bull.Am.Phys.Soc. 5, No.2, 110, N3 (1960) T.Retz-Schmidt, T.W.Bonner, G.U.Din, J.L.Weil Absolute Yields of Neutron Groups from Be9(α, n)C12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1960RE07 Phys.Rev. 119, 1079 (1960) Excitation Curves and Angular Distributions for N14(d, n)O15 NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.119.1079
1959WE33 Bull.Am.Phys.Soc. 4, No.8, 444, C8 (1959) N14(d, n)O15 Excitation Curves and Angular Distributions
1958JO28 Phys.Rev. 112, 1252 (1958) K.W.Jones, L.J.Lidofsky, J.L.Weil N15(p, n)O15 Reaction Study
doi: 10.1103/PhysRev.112.1252
1958JO29 Phys.Rev.Letters 1, 391 (1958) K.W.Jones, L.J.Lidofsky, J.L.Weil N15(p, n)O15 Reaction Study
doi: 10.1103/PhysRevLett.1.391
1958WE26 Phys.Rev. 110, 466 (1958) Total Neutron Cross Sections of Mg, Al, Fe, Cu, Zn, Mo, and Pb from 4 to 8 MeV
doi: 10.1103/PhysRev.110.466
1958WE31 Phys.Rev. 112, 1975 (1958) N14(d, n)O15 and N15(d, n)O16 Reactions
doi: 10.1103/PhysRev.112.1975
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