NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = K.T.Lesko Found 59 matches. 2021AK04 Phys.Rev. C 104, 065501 (2021) D.S.Akerib, A.K.Al Musalhi, S.K.Alsum, C.S.Amarasinghe, A.Ames, T.J.Anderson, N.Angelides, H.M.Araujo, J.E.Armstrong, M.Arthurs, X.Bai, J.Balajthy, S.Balashov, J.Bang, J.W.Bargemann, D.Bauer, A.Baxter, P.Beltrame, E.P.Bernard, A.Bernstein, A.Bhatti, A.Biekert, T.P.Biesiadzinski, H.J.Birch, G.M.Blockinger, E.Bodnia, B.Boxer, C.A.J.Brew, P.Bras, S.Burdin, J.K.Busenitz, M.Buuck, R.Cabrita, M.C.Carmona-Benitez, M.Cascella, C.Chan, N.I.Chott, A.Cole, M.V.Converse, A.Cottle, G.Cox, O.Creaner, J.E.Cutter, C.E.Dahl, L.de Viveiros, J.E.Y.Dobson, E.Druszkiewicz, S.R.Eriksen, A.Fan, S.Fayer, N.M.Fearon, S.Fiorucci, H.Flaecher, E.D.Fraser, T.Fruth, R.J.Gaitskell, J.Genovesi, C.Ghag, E.Gibson, S.Gokhale, M.G.D.van der Grinten, C.B.Gwilliam, C.R.Hall, S.J.Haselschwardt, S.A.Hertel, M.Horn, D.Q.Huang, M.C.I.gnarra, O.Jahangir, R.S.James, W.Ji, J.Johnson, A.C.Kaboth, A.C.Kamaha, K.Kamdin, K.Kazkaz, D.Khaitan, A.Khazov, I.Khurana, D.Kodroff, L.Korley, E.V.Korolkova, H.Kraus, S.Kravitz, L.Kreczko, B.Krikler, V.A.Kudryavtsev, E.A.Leason, J.Lee, D.S.Leonard, K.T.Lesko, C.Levy, J.Liao, J.Lin, A.Lindote, R.Linehan, W.H.Lippincott, X.Liu, M.I.Lopes, E.Lopez Asamar, B.Lopez Paredes, W.Lorenzon, S.Luitz, P.A.Majewski, A.Manalaysay, L.Manenti, R.L.Mannino, N.Marangou, M.E.McCarthy, D.N.McKinsey, J.McLaughlin, E.H.Miller, E.Mizrachi, A.Monte, M.E.Monzani, J.A.Morad, J.D.Morales Mendoza, E.Morrison, B.J.Mount, A.St.J.Murphy, D.Naim, A.Naylor, C.Nedlik, H.N.Nelson, F.Neves, J.A.Nikoleyczik, A.Nilima, I.Olcina, K.C.Oliver-Mallory, S.Pal, K.J.Palladino, J.Palmer, S.Patton, N.Parveen, E.K.Pease, B.Penning, G.Pereira, A.Piepke, Y.Qie, J.Reichenbacher, C.A.Rhyne, A.Richards, Q.Riffard, G.R.C.Rischbieter, R.Rosero, P.Rossiter, D.Santone, A.B.M.R.Sazzad, R.W.Schnee, P.R.Scovell, S.Shaw, T.A.Shutt, J.J.Silk, C.Silva, R.Smith, M.Solmaz, V.N.Solovov, P.Sorensen, J.Soria, I.Stancu, A.Stevens, K.Stifter, B.Suerfu, T.J.Sumner, N.Swanson, M.Szydagis, W.C.Taylor, R.Taylor, D.J.Temples, P.A.Terman, D.R.Tiedt, M.Timalsina, W.H.To, D.R.Tovey, M.Tripathi, D.R.Tronstad, W.Turner, U.Utku, A.Vaitkus, B.Wang, J.J.Wang, W.Wang, J.R.Watson, R.C.Webb, R.G.White, T.J.Whitis, M.Williams, F.L.H.Wolfs, D.Woodward, C.J.Wright, X.Xiang, J.Xu, M.Yeh, P.Zarzhitsky Projected sensitivity of the LUX-ZEPLIN experiment to the two-neutrino and neutrinoless double β decays of 134Xe RADIOACTIVITY 134Xe(2β-); measured recoiling nuclei and electrons, decay energy spectra using LUX-ZEPLIN (LZ) detector of liquid xenon (LXe), with scintillation and electro-luminescence light detected using 494 photomultipliers at Sanford Underground Research Facility (SURF) in South Dakota; deduced lower limits of T1/2 values for 2νββ and 0νββ decay modes.
doi: 10.1103/PhysRevC.104.065501
2015NO06 Appl.Radiat.Isot. 103, 177 (2015) E.B.Norman, T.E.Chupp, K.T.Lesko, P.J.Grant, G.L.Woodruff 19F(α, n) thick target yield from 3.5 to 10.0 MeV NUCLEAR REACTIONS 19F(n, α)1NN, E=3.5-10 MeV; measured reaction products, En, In; deduced thick-target yields. Comparison with available data.
doi: 10.1016/j.apradiso.2015.04.018
2012LE20 Eur.Phys.J.Plus 127, 107 (2012) The Sanford Underground Research Facility at Homestake
doi: 10.1140/epjp/i2012-12107-x
1998NO06 Phys.Rev. C57, 2010 (1998) E.B.Norman, E.Browne, Y.D.Chan, I.D.Goldman, R.-M.Larimer, K.T.Lesko, M.Nelson, F.E.Wietfeldt, I.Zlimen Half-Life of 44Ti RADIOACTIVITY 44Ti(EC) [from 45Sc(p, 2n), E=40 MeV]; measured Eγ, Iγ(t); deduced T1/2. Astrophysical implications.
doi: 10.1103/PhysRevC.57.2010
1997BA10 Phys.Rev. C55, 820 (1997) D.W.Bardayan, M.T.F.da Cruz, M.M.Hindi, A.F.Barghouty, Y.D.Chan, A.Garcia, R.-M.Larimer, K.T.Lesko, E.B.Norman, D.F.Rossi, F.E.Wietfeldt, I.Zlimen Radioisotope Yields from 1.85-GeV Protons on Mo and 1.85- and 5.0-GeV Protons on Te NUCLEAR REACTIONS Mo(p, X), E=1.85 GeV; Te(p, X), E=1.85, 5 GeV; measured Eγ, Iγ, σ; deduced effective yields for 74Br-116In isotopes.
doi: 10.1103/PhysRevC.55.820
1997HE11 Phys.Rev. C56, 922 (1997) R.K.Heaton, H.W.Lee, B.C.Robertson, E.B.Norman, K.T.Lesko, B.Sur α-Particle Induced γ-Ray Transitions in Light Elements NUCLEAR REACTIONS, ICPND 10B(α, p), (α, d), E=5.6-10 MeV; 11B(α, n), E=5.6-10 MeV; 19F(α, α'), (α, p), E=5.6-10 MeV; 23Na(α, n), (α, p), E=5.6-10 MeV; 24Mg(α, p), 25Mg(α, α'), (α, n), E ≤ 10 MeV; 26Mg(α, n), (α, p), E=5.6-10 MeV; 27Al(α, α'), E=10 MeV; 27Al(α, n), E=7-10 MeV; 27Al(α, p), E=5.6-10 MeV; 28Si(α, p), 29,30Si(α, n), (α, p), E=10 MeV; measured thick target residuals yields; deduced reaction mechanism related features. 28,29,30Si deduced excitation distribution vs Eα. Comparison of several models.
doi: 10.1103/PhysRevC.56.922
1997NO06 Nucl.Phys. A621, 92c (1997) E.B.Norman, E.Browne, Y.D.Chan, I.D.Goldman, R.-M.Larimer, K.T.Lesko, M.Nelson, F.E.Wietfeldt, I.Zlimen On the Half-Life of 44Ti RADIOACTIVITY 44Ti(EC); measured T1/2.
doi: 10.1016/S0375-9474(97)00218-2
1996EJ03 Phys.Rev. C54, 2047 (1996) R.Ejnisman, I.D.Goldman, P.R.Pascholati, M.T.F.da Cruz, R.M.Oliveira, E.B.Norman, I.Zlimen, F.E.Wietfeldt, R.M.Larimer, Y.D.Chan, K.T.Lesko, A.Garcia Cross Sections for 45Sc(p, 2n)44Ti and Related Reactions NUCLEAR REACTIONS, ICPND 45Sc(p, 2n), (p, np), (p, n), (p, n3p), (p, 3p), E=16-55 MeV; measured Eγ, Iγ following irradiation; deduced σ(E). Ge detectors, stacked foil technique.
doi: 10.1103/PhysRevC.54.2047
1996IS07 Nucl.Phys.(Proc.Suppl.) S48, 244 (1996) M.C.P.Isaac, Y.D.Chan, D.Hurley, K.T.Lesko, R.J.McDonald, M.E.Moorhead, E.B.Norman, A.R.Smith, R.G.Stokstad Preliminary Results from a Study of the Double Beta Decay of 150Nd RADIOACTIVITY 150Nd(2β); measured Eγ, Iγ followed 2ν-accompanied 2β-decay; deduced T1/2 lower limit for decay to 0+ state in 150Sm.
doi: 10.1016/0920-5632(96)00251-4
1995HE40 Nucl.Instrum.Methods Phys.Res. A364, 317 (1995) R.K.Heaton, H.W.Lee, B.C.Robertson, E.B.Norman, K.T.Lesko, B.Sur α-Particle Induced High-Energy γ-Ray Yields from Light Elements NUCLEAR REACTIONS, ICPND 27Al, 24Mg, 10B, 19F(α, p), 10B(α, d), 11B, 19F, 25,26Mg, 27Al(α, n), E=5.6-10 MeV; measured thick target γ yields; deduced γ production intensity distributions from materials related features. Thick targets of Be also studied.
doi: 10.1016/0168-9002(95)00220-0
1995NO05 Phys.Lett. 357B, 521 (1995) E.B.Norman, B.Sur, K.T.Lesko, R.-M.Larimer, D.J.DePaolo, T.L.Owens An Improved Test of the Exponential Decay Law RADIOACTIVITY 40K(β-), (EC); measured Eγ, Iγ, decay rate; deduced exponential decay law validity. Fresh, 'old' samples.
doi: 10.1016/0370-2693(95)00818-6
1995PA50 Nucl.Instrum.Methods Phys.Res. B100, 464 (1995) R.L.Paul, L.J.Harris, P.A.J.Englert, I.D.Goldman, C.Jackson, R.-M.Larimer, K.T.Lesko, B.Napier, E.B.Norman, B.Sur Production of Cosmogenic Nuclides in Thick Targets by Alpha Bombardment. Part I - Short-Lived Radioisotopes NUCLEAR REACTIONS C, Mg, 27Al, Si, O, Fe, Ne, Ge(α, X), E=60-120 MeV; measured production yield for residuals from 7Be to 65Zn; deduced cosmogenic nuclides production related features.
doi: 10.1016/0168-583X(95)00355-X
1995WI20 Phys.Rev. C52, 1028 (1995) F.E.Wietfeldt, E.B.Norman, Y.D.Chan, M.T.F.da Cruz, A.Garcia, E.E.Haller, W.L.Hansen, M.M.Hindi, R.-M.Larimer, K.T.Lesko, P.N.Luke, R.G.Stokstad, B.Sur, I.Zlimen Further Studies on the Evidence for a 17-keV Neutrino in a 14C-Doped Germanium Detector RADIOACTIVITY 14C(β-); measured β-endpoint energy; deduced Qβ, no 17 keV neutrino evidence. Source doping of Ge detector.
doi: 10.1103/PhysRevC.52.1028
1994HI05 Phys.Rev. C50, 728 (1994) M.M.Hindi, A.E.Champagne, M.T.F.da Cruz, R.-M.Larimer, K.T.Lesko, E.B.Norman, B.Sur β+ Decay and Cosmic-Ray Half-Lives of 143Pm and 144Pm RADIOACTIVITY 143,144Pm(β+) [from Pr(α, X), E=30 MeV]; measured Eγ, Iγ, annihilation γγ-coin; deduced β+-branching upper limits, partial T1/2 estimates.
doi: 10.1103/PhysRevC.50.728
1993DA19 Phys.Rev. C48, 3106 (1993) M.T.F.da Cruz, D.W.Bardayan, Y.Chan, A.Garcia, M.M.Hindi, R.-M.Larimer, K.T.Lesko, E.B.Norman, D.F.Rossi, R.G.Stokstad, F.E.Wietfeldt, I.Zlimen Thick-Target Yields of Iodine Isotopes from Proton Interactions in Te, and the Double-β Decays of 128,130Te NUCLEAR REACTIONS, ICPND 126,128,130Te(p, xn)126I/128I/130I, E=15-50 MeV; measured thick target residuals yields. 126,128,130Te(p, xn)126I/128I/130I, E=1.85, 5 GeV; measured residuals production σ; deduced revised correction for cosmic ray production of 126,128,130Xe ores, 120,128Te 2β-decay T1/2 implications. Activation technique, Ge detector.
doi: 10.1103/PhysRevC.48.3106
1993DA20 Phys.Rev. C48, 3110 (1993) M.T.F.da Cruz, Y.Chan, A.Garcia, M.M.Hindi, G.Kenchian, R.-M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, F.E.Wietfeldt, I.Zlimen Search for the β+ Decay of 54Mn RADIOACTIVITY 54Mn(β+); measured γγ-coin; deduced log ft. 54Cr levels deduced Iβ+ limit. Source as cosmic ray chronometer discussed. Hyperpure Ge detectors.
doi: 10.1103/PhysRevC.48.3110
1993GA09 Phys.Rev. C47, 2910 (1993) A.Garcia, Y.-D.Chan, M.T.F.da Cruz, R.M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, F.E.Wietfeldt, I.Zlimen, D.M.Moltz, J.Batchelder, T.J.Ognibene, M.M.Hindi Electron-Capture Decay of 100Tc and the Double-β Decay of 100Mo RADIOACTIVITY 100Tc(EC) [from 100Mo(p, n), E=9 MeV]; measured Eγ, Iγ, E X-ray, I X-ray; deduced log ft, T1/2. 100Mo deduced two-step process role in 2ν-accompanied 2β-decay, T1/2.
doi: 10.1103/PhysRevC.47.2910
1993HI09 Phys.Rev. C47, 2598 (1993) M.M.Hindi, B.Sur, K.L.Wedding, D.W.Bardayan, K.R.Czerwinski, M.T.F.da Cruz, D.C.Hoffman, R.-M.Larimer, K.T.Lesko, E.B.Norman β+ Decay and Cosmic-Ray Half-Life of 91Nb RADIOACTIVITY 91,91mNb(β+), (EC); measured Eγ, Iγ, E X-ray, I X-ray; deduced β-branching ratios, partial T1/2; deduced EC capture rates. Chemically purified sample source.
doi: 10.1103/PhysRevC.47.2598
1993WI05 Phys.Rev.Lett. 70, 1759 (1993) F.E.Wietfeldt, Y.D.Chan, M.T.F.da Cruz, A.Garcia, R.-M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, I.Zlimen Search for a 17 keV Neutrino in the Electron-Capture Decay of 55Fe RADIOACTIVITY 55Fe(EC); measured internal bremsstrahlung γ spectra; deduced no evidence for 5-25 keV mass neutrino. Chemically purified 55Fe sample, coaxial Ge detector.
doi: 10.1103/PhysRevLett.70.1759
1992DA15 Phys.Rev. C46, 1132 (1992) M.T.F.da Cruz, Y.Chan, R.-M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, F.E.Wietfeldt, I.Zlimen Half-Life of 56Ni RADIOACTIVITY 56Ni(EC) [from 56Fe(3He, 3n), E=50 MeV]; measured Eγ, Iγ, time dependent γ yields; deduced T1/2.
doi: 10.1103/PhysRevC.46.1132
1992SI11 Z.Phys. A341, 249 (1992) B.Singh, H.W.Taylor, E.Browne, H.L.Hall, E.B.Norman, R.M.Larimer, A.O.Macchiavelli, K.T.Lesko, B.Sur Study of γ Radiation from 100Pd Decay RADIOACTIVITY 100Pd(EC) [from 103Rh(p, 4n), E=45 MeV]; measured Eγ, Iγ, γγ-, γ(X-ray)-coin. 100Rh deduced levels.
doi: 10.1007/BF01283532
1992SU03 Phys.Rev.Lett. 68, 1435 (1992) B.Sur, E.B.Norman, F.E.Wietfeldt, K.T.Lesko, M.M.Hindi, R.-M.Larimer, P.N.Luke, W.L.Hansen, E.E.Haller Sur et al. Reply: RADIOACTIVITY 109Cd, 57Co, 139Ce; measured photoelectron spectra; deduced no satellite peaks, no coherent radiation evidence. 14C doped Ge detector.
doi: 10.1103/PhysRevLett.68.1435
1992ZL01 Phys.Rev. C46, 1136 (1992) I.Zlimen, E.Browne, Y.Chan, M.T.F.da Cruz, A.Garcia, R.-M.Larimer, K.T.Lesko, E.B.Norman, R.G.Stokstad, F.E.Wietfeldt Second-Forbidden Electron-Capture Decay of 55Fe RADIOACTIVITY 55Fe(EC); measured I gamma; deduced log ft, decay characteristics. 55Mn level deduced branching.
doi: 10.1103/PhysRevC.46.1136
1991LE28 Phys.Rev. C44, 2850 (1991) K.T.Lesko, E.B.Norman, R.-M.Larimer, B.Sur, C.B.Beausang 176Lu: An unreliable s-process chronometer NUCLEAR REACTIONS 176Yb(p, n), E=8 MeV; measured Eγ, γγ-coin; deduced astrophysical s-process chronometer, thermometer applications. 176Lu deduced levels, J, π.
doi: 10.1103/PhysRevC.44.2850
1991NO07 J.Phys.(London) G17, S291 (1991) E.B.Norman, B.Sur, K.T.Lesko, M.M.Hindi, R.-M.Larimer, T.R.Ho, J.T.Witort, P.N.Luke, W.L.Hansen, E.E.Haller Evidence for the Emission of a Massive Neutrino in Nuclear Beta Decay RADIOACTIVITY 14C(β-); measured β-spectra; deduced heavy neutrino evidence, mass, emission probability. 55Fe(EC); measured inner bremsstrahlung spectrum.
doi: 10.1088/0954-3899/17/S/031
1991SU09 Phys.Rev.Lett. 66, 2444 (1991) B.Sur, E.B.Norman, K.T.Lesko, M.M.Hindi, R.-M.Larimer, P.N.Luke, W.L.Hansen, E.E.Haller Evidence for the Emission of a 17-keV Neutrino in the β Decay of 14C RADIOACTIVITY 14C; measured β-spectra; deduced heavy neutrino evidence, mass, emission probability. Ge detector.
doi: 10.1103/PhysRevLett.66.2444
1990DI10 Phys.Rev. C42, 2108 (1990) D.E.DiGregorio, K.T.Lesko, B.A.Harmon, E.B.Norman, J.Pouliot, B.Sur, Y.Chan, R.G.Stokstad Angular Momentum in Sub-Barrier Fusion: Experimental study using the isomer ratio 137mCe/137gCe NUCLEAR REACTIONS, ICPND 128Te(12C, 3n), 133Cs(7Li, 3n), 137,136Ba(3He, 2n), 136Ba(α, 3n), 137Ba(3He, 3n), E=2.7-9.5 MeV/nucleon; measured 137mCe/137gCe isomer ratio, 3n, 2n reaction σ(E); deduced absolute average angular momentum for fusion. Coupled-channels model, statistical decay model calculations. Activation technique.
doi: 10.1103/PhysRevC.42.2108
1990GU20 Phys.Rev.Lett. 65, 2523 (1990) J.H.Gundlach, K.A.Snover, J.A.Behr, C.A.Gossett, M.Kicinska-Habior, K.T.Lesko Oblate Deformed Shapes of Hot Rotating Nuclei Deduced from Giant-Dipole-Resonance Decay Studies NUCLEAR REACTIONS 72Ge(18O, X), E=50, 74 MeV; 64Ni(28Si, X), E=137 MeV; measured Eγ, Iγ, σ(Eγ), γ(θ). 90Zr, 92Mo deduced GDR parameters, shape features. Hot rotating nuclei.
doi: 10.1103/PhysRevLett.65.2523
1990SU13 Phys.Rev. C42, 573 (1990) B.Sur, E.B.Norman, K.T.Lesko, E.Browne, R.-M.Larimer Reinvestigation of 56Ni Decay RADIOACTIVITY 56Ni(EC), (β+) [from 56Fe(3He, n), E=50 MeV]; measured Eγ, Iγ; deduced log ft. 56Co levels deduced relative Iγ, EC-branching, β+ branching ratio upper limit.
doi: 10.1103/PhysRevC.42.573
1989BR24 Nucl.Phys. A501, 477 (1989) E.Browne, B.Sur, E.B.Norman, H.L.Hall, R.A.Henderson, K.T.Lesko, R.M.Larimer, D.C.Hoffman Nuclear Penetration Effects in 233U RADIOACTIVITY 233Pa(β-) [from 237Np(α decay)]; measured Eγ, Iγ, I(ce), Iβ. 233U deduced transitions ICC, nuclear penetration parameter λ.
doi: 10.1016/0375-9474(89)90142-5
1989LE01 Phys.Rev. C39, 619 (1989) K.T.Lesko, E.B.Norman, R.-M.Larimer, J.C.Bacelar, E.M.Beck Level Scheme of 148Pm and the s-Process Neutron Density NUCLEAR REACTIONS 148Nd(p, nγ), E=8 MeV; measured I(γ), E(γ), γγ-coin; deduced s-process neutron density. 148Pm deduced levels.
doi: 10.1103/PhysRevC.39.619
1989LE17 Phys.Rev. C40, 445 (1989) K.T.Lesko, E.B.Norman, B.Sur, R.-M.Larimer Half-Life of 56Co RADIOACTIVITY 56Co(EC), (β+); measured T1/2, Eγ, Iγ. Time-dependent γ-yield measurement.
doi: 10.1103/PhysRevC.40.445
1989ST02 Phys.Rev.Lett. 62, 399 (1989) R.G.Stokstad, D.E.DiGregorio, K.T.Lesko, B.A.Harmon, E.B.Norman, J.Pouliot, Y.D.Chan Observation of a Constant Average Angular Momentum for Fusion at Sub-Barrier Energies NUCLEAR REACTIONS, ICPND 128Te(12C, 3n), E(cm)=34.5-50 MeV; measured σ(E); deduced isomer ratio.
doi: 10.1103/PhysRevLett.62.399
1989SU08 Phys.Rev. C39, 1511 (1989) B.Sur, K.R.Vogel, E.B.Norman, K.T.Lesko, R.-M.Larimer, E.Browne β+ Decay and Cosmic-Ray Half-Life of 54Mn RADIOACTIVITY 54Mn(β+), (β-); measured E(β+), I(β+); deduced β+ branching ratio upper limits, β+ partial T1/2 lower limits, second forbidden unique log ft, β--partial T1/2.
doi: 10.1103/PhysRevC.39.1511
1988GA02 Phys.Rev.Lett. 60, 499 (1988) J.D.Garnett, E.D.Commins, K.T.Lesko, E.B.Norman β-Decay Asymmetry Parameter for 35Ar: An anomaly resolved RADIOACTIVITY 35Ar(β+), (EC) [from 35Cl(polarized p, n), E=10 MeV]; measured β-decay asymmetry parameter; deduced quark mixing angle.
doi: 10.1103/PhysRevLett.60.499
1988LE08 Phys.Rev. C37, 1808 (1988) K.T.Lesko, E.B.Norman, R.-M.Larimer, S.Kuhn, D.M.Meekhof, S.G.Crane, H.G.Bussell Measurements of Cross Sections Relevant to γ-Ray Line Astronomy NUCLEAR REACTIONS, ICPND C, N, O, Mg, 27Al, Si, Fe(p, xnypzα), E=8.9-50 MeV; measured γ-production σ(E).
doi: 10.1103/PhysRevC.37.1808
1988NO02 Phys.Rev. C37, 860 (1988) E.B.Norman, K.T.Lesko, A.E.Champagne Low-Lying Levels in 148Pm NUCLEAR REACTIONS 149Sm(d, 3He), E=27.7 MeV; measured σ(E(3He)); deduced astrophysical implications. 148Pm deduced levels. Enriched targets, Q3D spectrograph.
doi: 10.1103/PhysRevC.37.860
1988VA01 Phys.Rev. C37, 178 (1988) A.M.van den Berg, W.Henning, L.L.Lee, K.T.Lesko, K.E.Rehm, J.P.Schiffer, G.S.F.Stephans, F.L.H.Wolfs, W.S.Freeman Quasi-Elastic Processes in 58Ni- and 64Ni-Induced Reactions on Sn Isotopes NUCLEAR REACTIONS 112,116,120,124Sn(58Ni, 58Ni), (58Ni, 58Ni'), (58Ni, X), E=330 MeV; 112,116,120,124Sn(64Ni, 64Ni), (64Ni, 64Ni'), (64Ni, X), E=341, 380 MeV; 112Sn(58Ni, 59Ni), (58Ni, 57Ni), E=330 MeV; measured quasielastic σ(θ); deduced quasielastic, reaction σ.
doi: 10.1103/PhysRevC.37.178
1987HI10 Phys.Rev. C36, 989 (1987) J.D.Hinnefeld, J.J.Kolata, D.J.Henderson, R.V.F.Janssens, D.G.Kovar, K.T.Lesko, G.Rosner, G.S.F.Stephans, A.M.Van Den Berg, B.D.Wilkins, F.W.Prosser, S.V.Reinert, P.L.Gonthier Velocity and Angular Distributions of Evaporation Residues from 32S-Induced Reactions NUCLEAR REACTIONS 12C, 24Mg, 27Al, 28Si, 40Ca(32S, X), E=194, 239, 278 MeV; measured evaporation residue spectra, σ(fragment θ). 24Mg(32S, 32S), E=194, 239, 278 MeV; measured σ(θ); deduced σ(E), complete fusion limitations.
doi: 10.1103/PhysRevC.36.989
1986JA16 Phys.Lett. 181B, 16 (1986) R.V.F.Janssens, R.Holzmann, W.Henning, T.L.Khoo, K.T.Lesko, G.S.F.Stephans, D.C.Radford, A.M.van den Berg, W.Kuhn, R.M.Ronningen Evaporation Residue Cross Sections and Average Neutron Multiplicities in the 64Ni + 92Zr and 12C + 144Sm Reactions leading to 156Er NUCLEAR REACTIONS, ICPND 144Sm(12C, X), E=50-90 MeV; 92Zr(64Ni, X), E=200-300 MeV; measured evaporation residue σ(E), neutron multipicities; calculated fusion σ. ΔE-E detector. Statistical model calculations.
doi: 10.1016/0370-2693(86)91245-1
1986LE18 Phys.Rev. C34, 2155 (1986) K.T.Lesko, W.Henning, K.E.Rehm, G.Rosner, J.P.Schiffer, G.S.F.Stephans, B.Zeidman, W.S.Freeman Fission following Fusion of Ni + Sn NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(58Ni, X), (58Ni, F), (64Ni, X), (64Ni, F), E(cm)=150-240 MeV; measured fission, fusion σ(E); deduced statistical, extra push model parameters.
doi: 10.1103/PhysRevC.34.2155
1986LE19 Phys.Rev. C34, 2256 (1986) K.T.Lesko, E.B.Norman, D.M.Moltz, R.M.Larimer, S.G.Crane, S.E.Kellogg Isomeric Levels in 180Lu and the Nucleosynthesis of 180mTa RADIOACTIVITY 180Lu(β-) [from 180Hf(n, p)]; measured Eγ, Iγ, T1/2; deduced 180mTa nucleosynthesis consequences. 180Lu deduced isomer T1/2, production σ. Enriched targets, rabbit transfer system, Ge detector.
doi: 10.1103/PhysRevC.34.2256
1986NO05 Radiat.Eff. 94, 307 (1986) E.B.Norman, K.T.Lesko, T.E.Chupp, P.Schwalbach, M.A.Faccio Gamma-Ray Production Cross Sections for Alpha-Particle Induced Reactions on 19F and 23Na NUCLEAR REACTIONS 23Na, 19F(α, γ), E=4.5-26 MeV; measured Eγ, Iγ, γ production σ(E). Ge(Li) detector, NaF target.
doi: 10.1080/00337578608208398
1986RA08 Phys.Rev.Lett. 57, 815 (1986) A.Ray, D.D.Leach, R.Vandenbosch, K.T.Lesko, D.Shapira Nonequilibrium Population of Magnetic Substates and Excitation-Energy Division in the Decay of an Orbiting Complex NUCLEAR REACTIONS 12C(28Si, 12C), E(cm)=42.7, 33.7 MeV; measured γγ(θ), (particle)γ-coin, Eγ, Iγ; deduced orbiting complex decay excitation energy division. 12C level deduced m=0 magnetic substate production.
doi: 10.1103/PhysRevLett.57.815
1986SA25 Phys.Rev. C34, 1746 (1986) S.J.Sanders, R.R.Betts, I.Ahmad, K.T.Lesko, S.Saini, B.D.Wilkins, F.Videbaek, B.K.Dichter Fission-Like Yields in 16O + 40,44Ca Reactions NUCLEAR REACTIONS 40,44Ca(16O, X), E=69.3-87.3 MeV; measured σ(E, θ) vs mass, evaporation residue yields; deduced fusion σ(E). Enriched target, tof. Deep-inelastic scattering calculations.
doi: 10.1103/PhysRevC.34.1746
1986VA01 Phys.Rev.Lett. 56, 572 (1986) A.M.van den Berg, W.Henning, L.L.Lee, Jr., K.T.Lesko, K.E.Rehm, J.P.Schiffer, G.S.F.Stephans, F.L.H.Wolfs, W.S.Freeman Quasielastic Nucleon Transfer and the Heavy-Ion Interaction Potential NUCLEAR REACTIONS 112Sn(58Ni, 58Ni), (58Ni, 58Ni'), (58Ni, 59Ni), (58Ni, 57Ni), (58Ni, 60Ni), E=330 MeV; measured σ(θ). 112,116,120,124Sn(58Ni, X), E=330 MeV; 112,116,120,124Sn(64Ni, X), E=341 MeV; measured reaction σ for fragment Z=24-29; deduced quasielastic process role in nucleus-nucleus potential.
doi: 10.1103/PhysRevLett.56.572
1985LE13 Phys.Rev.Lett. 55, 803 (1985) K.T.Lesko, W.Henning, K.E.Rehm, G.Rosner, J.P.Schiffer, G.S.F.Stephans, B.Zeidman, W.S.Freeman Fission and Particle Decay of Cold Compound Nuclei with High Angular Momentum NUCLEAR REACTIONS 124,118,112Sn(58Ni, F), (64Ni, F), (58Ni, X), (64Ni, X), E=200-380 MeV; measured fission, evaporation residue σ vs E; deduced fission, light particle emission competition. Statistical model.
doi: 10.1103/PhysRevLett.55.803
1985MA10 Phys.Rev. C31, 867 (1985) J.F.Mateja, A.D.Frawley, D.G.Kovar, D.Henderson, H.Ikezoe, R.V.F.Janssens, G.Rosner, G.S.F.Stephans, B.Wilkins, K.T.Lesko, M.F.Vineyard 10B + 13C and 11B + 12C Reactions from 4 to 9 MeV/Nucleon NUCLEAR REACTIONS, ICPND 12C(11B, X), (11B, 11B), 13C(10B, 10B), (10B, X), E=4-9 MeV/nucleon; measured σ(θ), σ(fragment E) for fragment mass=15, 20, 11, 6, fusion σ vs E; deduced nonfusion σ for mass 6-13, entrance channel role in fusion. 23Na deduced critical L vs excitation energy.
doi: 10.1103/PhysRevC.31.867
1985ST20 Phys.Lett. 161B, 60 (1985) G.S.F.Stephans, D.G.Kovar, R.V.F.Janssens, G.Rosner, H.Ikezoe, B.Wilkins, D.Henderson, K.T.Lesko, J.J.Kolata, C.K.Gelbke, B.V.Jacak, Z.M.Koenig, G.D.Westfall, A.Szanto De Toledo, E.M.Szanto, P.L.Gonthier Influence of Nucleon Fermi Motion on Incomplete Fusion NUCLEAR REACTIONS 24Mg, 27Al, 28Si, 40Ca, 48Ti(14N, X), E=5-35 MeV/nucleon; measured evaporation residue velocity spectra; deduced Fermi motion role in inelastic fusion. Other data input.
doi: 10.1016/0370-2693(85)90609-4
1984HI13 Nucl.Instrum.Methods 227, 434 (1984) G.M.Hinn, E.B.Norman, T.E.Chupp, K.T.Lesko Production of Thick Elemental Low-Oxygen Content (nat)Mg, 26Mg from (nat)MgO, 26MgO NUCLEAR REACTIONS Mg(α, γ), E=16 MeV; measured Eγ, Iγ. Mg, MgO targets.
doi: 10.1016/0168-9002(84)90199-2
1984NO07 Phys.Rev. C30, 1339 (1984) E.B.Norman, T.E.Chupp, K.T.Lesko, P.J.Grant, G.L.Woodruff 22Na Production Cross Sections from the 19F(α, n) Reaction NUCLEAR REACTIONS, ICPND 19F(α, n), E = 3.5-10 MeV; measured thick target neutron yield; deduced 22Na production cross sections. 3He filled proportional counter imbedded in graphite neutron detector. Hauser-Feshbach analysis.
doi: 10.1103/PhysRevC.30.1339
1983LE10 Phys.Rev. C27, 2999 (1983) K.T.Lesko, S.Gil, A.Lazzarini, V.Metag, A.G.Seamster, R.Vandenbosch Properties of Fission Induced by the Complete Capture of 40Ar by 238U at E(c.m.) = 291 MeV NUCLEAR REACTIONS 238U(40Ar, F), E(cm)=291 MeV; measured fission fragment σ(θ); deduced complete capture induced fission characteristics. Rotating liquid drop model.
doi: 10.1103/PhysRevC.27.2999
1983NO03 Phys.Rev. C27, 1728 (1983); Erratum Phys.Rev. C28, 1409 (1983) E.B.Norman, T.E.Chupp, K.T.Lesko, J.L.Osborne, P.J.Grant, G.L.Woodruff 7Be Decay Scheme and the Solar Neutrino Problem RADIOACTIVITY 7Be(EC) [from 7Li(p, n), E=1.9, 2.1, 3.5 MeV]; measured Iγ. 7Li level deduced EC-branching ratio.
doi: 10.1103/PhysRevC.27.1728
1982LE04 Phys.Rev. C25, 872 (1982) K.T.Lesko, D.-K.Lock, A.Lazzarini, R.Vandenbosch, V.Metag, H.Doubre Energy Dependence of Fusion Cross Section for 28Si + 12C by Evaporation Residue Measurements NUCLEAR REACTIONS, ICPND 28Si(12C, X)35Cl/38K/37Ar/34Cl/32S/34S/35Ar/35Cl/38Ar/31P, E(cm)=18.4-35 MeV; measured Eγ, Iγ, σ(evaporation residue) vs θ; deduced evaporation residual σ, fusion σ(E). Entrance channel, level density limitation models.
doi: 10.1103/PhysRevC.25.872
1982NO11 Nucl.Phys. A390, 561 (1982) E.B.Norman, T.E.Chupp, K.T.Lesko, P.Schwalbach, P.J.Grant 26g,26mAl Production Cross Sections from the 23Na(α, n)26Al Reaction NUCLEAR REACTIONS, ICPND 23Na(α, n), E=3.5-26 MeV; measured σ(E, Eγ, θ); deduced production σ for 26g,26mAl. Ge(Li), neutron, Nal detectors.
doi: 10.1016/0375-9474(82)90283-4
1981LA08 Phys.Rev. C24, 309 (1981) A.Lazzarini, H.Doubre, K.T.Lesko, V.Metag, A.Seamster, R.Vandenbosch, W.Merryfield Search for a Fusion L Window in the 16O + 16O System at E(cm) = 34 MeV NUCLEAR REACTIONS 16O(16O, 16O'), E(cm)=34 MeV; measured σ(θ); deduced single, double excitation dominance. Comparison with TDHF.
doi: 10.1103/PhysRevC.24.309
1981NO03 Nucl.Phys. A357, 228 (1981) E.B.Norman, K.T.Lesko, T.E.Chupp, P.Schwalbach 26Al Production Cross Sections from the 26Mg(p, n)26Al Reaction NUCLEAR REACTIONS 26Mg(p, n), E=5.45-14 MeV; measured σ(E, Eγ, θ); deduced production σ for 26Al(g.s.). Ge(Li) detector. 26Al(n, p), E=0.1-10 MeV; calculated σ(E); deduced production σ for 26Mg(g.s.). Detailed balance.
doi: 10.1016/0375-9474(81)90635-7
1981NO14 Astrophys.J. 251, 834 (1981) E.B.Norman, T.E.Chupp, K.T.Lesko, P.J.Grant Cross Sections for the 26Mg + p → 26Al + n and 26Al + n → 26Mg + p Reactions NUCLEAR REACTIONS 26Mg(p, n), E=threshold-7 MeV; measured σ(E); deduced σ for inverse reaction, nucleosynthesis of 26Al. Thick target yield technique.
doi: 10.1086/159527
1980SN01 Phys.Rev.Lett. 44, 927 (1980) K.A.Snover, P.G.Ikossi, E.G.Adelberger, K.T.Lesko Unique Determination of the Amplitude and Phase for the Population of The Giant-Dipole Resonance in the Reaction 12C(p(pol), γ0)13N NUCLEAR REACTIONS 12C(polarized p, γ), E=5-30 MeV; measured σ(E). 13N deduced GDR, T=3/2 M1(E2) interference.
doi: 10.1103/PhysRevLett.44.927
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