NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = C.R.Gould Found 95 matches. 2014GO24 Nucl.Data Sheets 118, 585 (2014) C.R.Gould, E.I.Sharapov, A.A.Sonzogni Nuclear Data and the Oklo Natural Nuclear Reactors NUCLEAR REACTIONS 138,140La, 175Lu, 235,238U(n, γ), E=reactor;175Lu(n, γ) measured Eγ, Iγ in Oklo reactor zone; deduced γ fluxes, 138La abundance, La concentration.
doi: 10.1016/j.nds.2014.04.142
2012GO04 Phys.Rev. C 85, 024610 (2012) 176Lu/175Lu thermometry for the Oklo natural reactors: A new examination of old data NUCLEAR REACTIONS 175,176Lu(n, γ), E=5-25 keV; analyzed isomer branching ratio; deduced Oklo natural reactor operating temperature. Comparison with previous studies.
doi: 10.1103/PhysRevC.85.024610
2012GO10 Phys.Rev. C 86, 027601 (2012) La-138/139 isotopic data and neutron fluences for Oklo RZ10 reactor ATOMIC MASSES 138,139La; calculated dependence of 138La abundance on neutron fluence and primordial elemental lanthanum concentration from zone RZ10 of Okla natural reactor.
doi: 10.1103/PhysRevC.86.027601
2012GO23 Phys.Rev. C 86, 054602 (2012) C.R.Gould, E.I.Sharapov, A.A.Sonzogni γ-ray fluxes in Oklo natural reactors NUCLEAR REACTIONS 235U(n, F), E=THERMAL;calculated prompt, delayed, and equilibrium γ-ray fluxes in pulsed mode operation of Oklo zone RZ10. Implications for 176Lu/175Lu. Monte Carlo simulation.
doi: 10.1103/PhysRevC.86.054602
2006FO04 Phys.Rev. C 73, 034002 (2006) R.D.Foster, C.R.Gould, D.G.Haase, J.M.Kelley, D.M.Markoff, W.Tornow Measurement of the relative longitudinal spin-dependent total cross-section difference in (n(pol)) - (d(pol)) scattering NUCLEAR REACTIONS 2H(polarized n, n), E=1.18, 5.0, 6.88, 9.0 MeV; measured spin-dependent cross section difference. Polarized target, comparison with model predictions.
doi: 10.1103/PhysRevC.73.034002
2006GO23 Phys.Rev. C 74, 024607 (2006) C.R.Gould, E.I.Sharapov, S.K.Lamoreaux Time variability of α from realistic models of Oklo reactors NUCLEAR REACTIONS 149Sm(n, X), E=spectrum; analyzed σ, isotopic abundances in natural reactor; deduced limits on time dependence of fine structure constant.
doi: 10.1103/PhysRevC.74.024607
2005DA33 J.Res.Natl.Inst.Stand.Technol. 110, 485 (2005) E.D.Davis, C.R.Gould, G.E.Mitchell, E.I.Sharapov Bounds on Time Reversal Violation From Polarized Neutron Capture With Unpolarized Targets
doi: 10.6028/jres.110.075
2004DA03 Phys.Rev. C 69, 015501 (2004) E.D.Davis, C.R.Gould, G.E.Mitchell, E.I.Sharapov Bounds on P-odd T-odd interactions from polarized neutron capture with unpolarized targets
doi: 10.1103/PhysRevC.69.015501
2002TO10 Phys.Rev. C65, 047002 (2002) W.Tornow, C.R.Gould, D.G.Haase, J.R.Walston, B.W.Raichle Double Polarized Neutron-Proton Scattering and Nucleon-Nucleon Tensor Force: An alternative analysis NUCLEAR REACTIONS 1H(polarized n, X), E=7.4-17.1 MeV; analyzed polarization observables; deduced mixing parameter, tensor force strength. Polarized target.
doi: 10.1103/PhysRevC.65.047002
2001WA01 Phys.Rev. C63, 014004 (2001) J.R.Walston, C.R.Gould, D.G.Haase, B.W.Raichle, M.L.Seely, W.Tornow, W.S.Wilburn, S.I.Penttila, G.W.Hoffmann Low-Energy NN Tensor Force from n(pol)-p(pol) Scattering: Results of an accurate experimental approach NUCLEAR REACTIONS 1H(polarized n, n), E=5-20 MeV; measured transverse, longitudinal relative σ; deduced mixing parameter, low-energy NN tensor force. Polarized target, comparisons with previous results.
doi: 10.1103/PhysRevC.63.014004
1999DA08 Phys.Lett. 447B, 209 (1999) Extraction of Bounds on Time-Reversal Non-Invariance from Neutron Reactions
doi: 10.1016/S0370-2693(99)00013-1
1999RA20 Phys.Rev.Lett. 83, 2711 (1999) B.W.Raichle, C.R.Gould, D.G.Haase, M.L.Seely, J.R.Walston, W.Tornow, W.S.Wilburn, S.I.Penttila, G.W.Hoffmann Double Polarized Neutron-Proton Scattering and Meson-Exchange Nucleon-Nucleon Potential Models NUCLEAR REACTIONS 1H(polarized n, X), E=5-20 MeV; measured longitudinal, transverse total σ differences; deduced phase-shift mixing parameter. Polarized target. Comparison with meson-exchange model predictions.
doi: 10.1103/PhysRevLett.83.2711
1998AD12 Rev.Mod.Phys. 70, 1265 (1998) E.G.Adelberger, S.M.Austin, J.B.Bahcall, A.B.Balantekin, G.Bogaert, L.S.Brown, L.Buchmann, F.E.Cecil, A.E.Champagne, L.de Braeckeleer, C.A.Duba, S.R.Elliott, S.J.Freedom, M.Gai, G.Goldring, C.R.Gould, A.Gruzinov, W.C.Haxton, K.M.Heeger, E.Henley, C.W.Johnson, M.Kamionkowski, R.W.Kavanagh, S.E.Koonin, K.Kubodera, K.Langanke, T.Motobayashi, V.Pandharipande, P.Parker, R.G.H.Robertson, C.Rolfs, R.F.Sawyer, N.Shaviv, T.D.Shoppa, K.A.Snover, E.Swanson, R.E.Tribble, S.Turck-Chieze, J.F.Wilkerson Solar Fusion Cross Sections NUCLEAR REACTIONS 7Be, 12,13C, 15N, 16,17,18O(p, γ), 14,15N, 17,18O(p, α), 7Li(d, p), 3He(p, e+), (α, γ), (3He, 2p), 1H(p, e+), E=low; compiled, analyzed S-factor data, calculations; deduced implications for solar neutrino flux calculations.
doi: 10.1103/RevModPhys.70.1265
1998DA02 Phys.Rev. C57, 648 (1998) On-Resonance Deformation Effect Measurements: A probe of order within chaos in the nucleus NUCLEAR REACTIONS 165Ho(n, X), E not given; calculated σ deformation effects; deduced oblate shape isomers role.
doi: 10.1103/PhysRevC.57.648
1998HU07 J.Phys.(London) G24, 763 (1998) P.R.Huffman, C.R.Gould, D.G.Haase The Deformation Effect and Time-Reversal Violation in Neutron Resonances NUCLEAR STRUCTURE 166Ho; calculated resonance wavefunctions; deduced deformation effect, test for time-reversal violation in neutron scattering.
doi: 10.1088/0954-3899/24/4/008
1998SE21 Phys.Rev. C58, 2977 (1998) S.J.Seestrom, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, M.Iinuma, J.N.Knudson, P.E.Koehler, L.Y.Lowie, A.Masaike, Y.Masuda, Y.Matsuda, G.E.Mitchell, S.I.Penttila, Yu.P.Popov, H.Postma, N.R.Roberson, E.I.Sharapov, H.M.Shimizu, D.A.Smith, S.L.Stephenson, Y.F.Yen, V.W.Yuan Parity Nonconservation in Neutron Capture on 113Cd NUCLEAR REACTIONS Cd, 113Cd(polarized n, γ), E=7-520 eV; measured Eγ, Iγ, transmission spectra, total capture σ helicity dependence. 113Cd deduced resonances J, π, widths, parity-violating asymmetries.
doi: 10.1103/PhysRevC.58.2977
1998WA19 Phys.Rev. C58, 1314 (1998) J.R.Walston, C.D.Keith, C.R.Gould, D.G.Haase, B.W.Raichle, M.L.Seely, W.Tornow, W.S.Wilburn, G.W.Hoffmann, S.I.Penttila Polarization Transfer in the 3H(p(pol), n(pol))3He Reaction and the 0- Level in 4He NUCLEAR REACTIONS 3H(polarized p, n), E=1.3-2.8 MeV; measured zero-degree polarization transfer coefficients. 4He deduced 0- level.
doi: 10.1103/PhysRevC.58.1314
1998WI25 Few-Body Systems 24, 27 (1998) W.S.Wilburn, C.R.Gould, G.M.Hale, P.R.Huffman, C.D.Keith, N.R.Roberson, W.Tornow Measurements at Low Energies of the Polarization-Transfer Coefficient Kyy' for the Reaction 3H(p(pol), n(pol))3He at 0° NUCLEAR REACTIONS 3H(polarized p, n), E=1.9, 5.2, 5.8 MeV; measured polarization transfer. Polarized neutron source application discussed. Comparison with R-matrix predictions.
doi: 10.1007/s006010050074
1997HU04 Phys.Rev. C55, 2684 (1997) P.R.Huffman, N.R.Roberson, W.S.Wilburn, C.R.Gould, D.G.Haase, C.D.Keith, B.W.Raichle, M.L.Seely, J.R.Walston Test of Parity-Conserving Time-Reversal Invariance using Polarized Neutrons and Nuclear Spin Aligned Holmium NUCLEAR REACTIONS 165Ho(n, n), E=5.9 MeV; measured time-reversal violating partial σ; deduced bound on parity-conserving time-reversal invariance in NN-interactions.
doi: 10.1103/PhysRevC.55.2684
1996HU05 Phys.Rev.Lett. 76, 4681 (1996) P.R.Huffman, N.R.Roberson, W.S.Wilburn, C.R.Gould, D.G.Haase, C.D.Keith, B.W.Raichle, M.L.Seely, J.R.Walston Test of Parity-Conserving Time-Reversal Invariance using Polarized Neutrons and Nuclear Spin Aligned Holmium NUCLEAR REACTIONS 165Ho(polarized n, X), E=5.9 MeV; measured transmission asymmetry, total σ difference for spin up/down; deduced T-violating spin correlation coefficient, bound on T-violating meson coupling. Nuclear spin aligned Holmium.
doi: 10.1103/PhysRevLett.76.4681
1996HU09 Phys.Rev. C54, 2051 (1996) P.R.Huffman, C.M.Frankle, C.R.Gould, D.G.Haase, J.A.Harvey, N.R.Roberson, L.W.Weston Neutron Resonances in 166Ho NUCLEAR REACTIONS 165Ho(n, X), E=epithermal; measured transmission spectra. 166Ho deduced resonances, 2gΓ(n), π.
doi: 10.1103/PhysRevC.54.2051
1996KE06 Phys.Rev. C54, 477 (1996) C.D.Keith, C.R.Gould, D.G.Haase, M.L.Seely, P.R.Huffman, N.R.Roberson, W.Tornow, W.S.Wilburn Measurements of the Total Cross Section for the Scattering of Polarized Neutrons from Polarized 3He NUCLEAR REACTIONS 3He(polarized n, n), E=1.95-7.45 MeV; measured longitudinal, transverse σ difference. Polarized 3He target. R-matrix, phase-shift analyses.
doi: 10.1103/PhysRevC.54.477
1995AL30 Nucl.Instrum.Methods Phys.Res. A352, 592 (1995) V.P.Alfimenkov, Yu.D.Mareev, V.V.Novitsky, L.B.Pikelner, V.R.Skoy, C.R.Gould, D.G.Haase, N.R.Roberson Measurements of Epithermal Neutron Depolarization using a Polarized Rare Earth Target
doi: 10.1016/0168-9002(95)90011-X
1995KE15 Nucl.Instrum.Methods Phys.Res. A357, 34 (1995) C.D.Keith, C.R.Gould, D.G.Haase, P.R.Huffman, N.R.Roberson, M.L.Seely, W.Tornow, W.S.Wilburn A Polarized Solid 3He Target for Neutron Transmission Experiments NUCLEAR REACTIONS 3He(polarized n, X), E=3.65 MeV; measured spin-spin transmission asymmetry. Polarized solid, liquid, warm liquid.
doi: 10.1016/0168-9002(94)01522-8
1995WI24 Phys.Rev. C52, 2351 (1995) W.S.Wilburn, C.R.Gould, D.G.Haase, P.R.Huffman, C.D.Keith, N.R.Roberson, W.Tornow Measurements of Δσ(T) in Polarized-Neutron-Polarized-Proton Scattering NUCLEAR REACTIONS 1H(polarized n, n), E=7.43, 9.57, 11.60 MeV; measured spin-dependent total σ difference; deduced 3S1-3D1 mixing parameter. Polarized target.
doi: 10.1103/PhysRevC.52.2351
1994EN06 Phys.Rev.Lett. 73, 3508 (1994) Microscopic T-Violating Optical Potential: Implications for neutron-transmission experiments NUCLEAR REACTIONS 165Ho(polarized n, X), E not given; calculated T-violating ρ-nucleon coupling limits, transmission experiments. Microscopic T-violating optical potential.
doi: 10.1103/PhysRevLett.73.3508
1994HN01 Phys.Rev. C49, R612 (1994) Optical-Model Description of Time-Reversal Violation in Neutron-Nucleus Scattering NUCLEAR REACTIONS 165Ho(n, n), E ≤ 20 MeV; calculated σ(E); 165Ho(polarized n, n), E ≤ 20 MeV; calculated T-odd spin-correlation coefficient vs E. Optical model.
doi: 10.1103/PhysRevC.49.R612
1994KE09 Phys.Rev. C50, 237 (1994) C.D.Keith, C.R.Gould, D.G.Haase, N.R.Roberson, W.Tornow, G.M.Hale, H.M.Hofmann, H.Postma Sensitivity of Polarized Neutron-Polarized 3He Scattering to the Excited Level Structure of 4He NUCLEAR REACTIONS 3He(polarized n, n), (n, n), E=0.1-10 MeV; calculated σ(E), total longitudinal, transverse σ differences; deduced sensitivity to 4He level structure. Multi-channel resonating group model, polarized target.
doi: 10.1103/PhysRevC.50.237
1994KO02 Phys.Rev. C49, 710 (1994) J.E.Koster, C.R.Gould, D.G.Haase, N.R.Roberson Spatial Orientation of Nuclei: Mass deformation in 165-Holmium NUCLEAR REACTIONS 165Ho(n, X), E=1.5, 1.8, 1.9, 3.9 MeV; measured transmission; deduced deformed optical model, quadrupole mass deformation parameters, total deformation σ(E). Cryogenically aligned rotating holmium single crystal target, coupled-channels analysis.
doi: 10.1103/PhysRevC.49.710
1993BO25 Phys.Rev. C48, 1116 (1993) J.D.Bowman, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, J.J.Yeh, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Experimental Limit on Parity Violation in Nonresonant Neutron-Nucleus Scattering NUCLEAR REACTIONS 232Th(polarized n, X), E=6-86 eV; measured transmission spectra, parity nonconserving longitudinal asymmetry; deduced nonresonant scattering parity violation limit.
doi: 10.1103/PhysRevC.48.1116
1993FR13 Phys.Rev. C48, 1601 (1993) C.M.Frankle, J.D.Bowman, B.E.Crawford, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.S.Patterson, S.I.Penttila, Yu.P.Popov, N.R.Roberson, S.J.Seestrom, E.I.Sharapov, Y.-F.Yen, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Neutron Resonance Spectroscopy of 113In and 115In NUCLEAR REACTIONS In(n, X), E=25-500 eV; measured transmission; deduced σ(E). 115In(n, γ), E=25-500 eV; measured capture Eγ, Iγ. 114,116In deduced resonances, parameters.
doi: 10.1103/PhysRevC.48.1601
1993FR19 Nucl.Instrum.Methods Phys.Res. B79, 306 (1993) C.M.Frankle, J.D.Bowman, J.N.Knudson, S.I.Penttila, S.J.Seestrom, S.H.Yoo, V.W.Yuan, C.R.Gould, D.G.Haase, G.E.Mitchell, N.R.Roberson, Yu.P.Popov, E.I.Sharapov, P.P.J.Delheij, H.Postma, and the TRIPLE Collaboration Measurement of Parity Violation in Compound Nuclear Resonances using Epithermal Polarized Neutrons NUCLEAR REACTIONS 81Br, 139La, 232Th, 238U(polarized n, X), E=epithermal; compiled, reviewed parity nonconserving analyzing power data.
doi: 10.1016/0168-583X(93)95351-5
1993HA39 Nucl.Instrum.Methods Phys.Res. B79, 300 (1993) D.G.Haase, J.D.Bowman, P.P.J.Delheij, C.M.Frankle, C.R.Gould, J.N.Knudson, J.E.Koster, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, S.H.Yoo, V.W.Yuan Bulk Magnetic Structure Studies using Polarized Epithermal Neutrons NUCLEAR REACTIONS Ho(polarized n, n), E=epithermal; measured neutron depolarization. Thick single ferromagnetic holmium crystal.
doi: 10.1016/0168-583X(93)95349-A
1993RO25 Nucl.Instrum.Methods Phys.Res. A326, 549 (1993) N.R.Roberson, C.D.Bowman, J.D.Bowman, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, R.N.Mortensen, S.I.Penttila, H.Postma, S.J.Seestrom, J.J.Szymanski, S.A.Wender, S.H.Yoo, V.W.Yuan, X.Zhu An Apparatus and Techniques of Tests for Fundamental Symmetries in Compound-Nucleus Scattering with Epithermal Polarized Neutron Beams NUCLEAR REACTIONS 238U(polarized n, X), E=5-300 eV; measured neutron transmission. 239U resonance deduced average parity violating asymmetry.
doi: 10.1016/0168-9002(93)90858-F
1993WI14 Phys.Rev.Lett. 71, 1982 (1993) W.S.Wilburn, C.R.Gould, D.G.Haase, P.R.Huffman, C.D.Keith, J.E.Koster, N.R.Roberson, W.Tornow Measurements of Polarized-Neutron-Polarized-Proton Scattering: Implication for the triton binding energy NUCLEAR REACTIONS 1H(polarized n, n), E=3.65-11.6 MeV; measured spin-dependent difference in σ; deduced tensor interaction magnitude, 3S1-3D1, mixing parameter, 3H binding energy implications.
doi: 10.1103/PhysRevLett.71.1982
1992BO01 Phys.Rev.Lett. 68, 780 (1992) J.D.Bowman, G.T.Garvey, C.R.Gould, A.C.Hayes, M.B.Johnson Parity Violation in the Compound Nucleus: The Role of Distant States NUCLEAR STRUCTURE 232Th; calculated parity violating asymmetry; deduced distant states role.
doi: 10.1103/PhysRevLett.68.780
1992FR14 Phys.Rev. C46, 778 (1992) C.M.Frankle, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Parity Nonconservation for Neutron Resonances in 232Th NUCLEAR REACTIONS 232Th(polarized n, X), E=6-400 eV; measured total σ, parity violating asymmetries. 233Th deduced resonances, p-wave parity nonconserving matrix element rms values, spreading width.
doi: 10.1103/PhysRevC.46.778
1992FR15 Phys.Rev. C46, 1542 (1992) C.M.Frankle, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Parity Nonconservation for the 0.88-eV Neutron Resonance in 81Br NUCLEAR REACTIONS 81Br(polarized n, n), E=0.88 eV; measured parity nonconserving longitudinal analyzing power, σ for p-wave resonances.
doi: 10.1103/PhysRevC.46.1542
1992KO09 Nucl.Instrum.Methods Phys.Res. A313, 464 (1992) J.E.Koster, C.R.Gould, D.G.Haase, N.R.Roberson A Rotating Aligned Holmium Target for Neutron Transmission Measurements NUCLEAR REACTIONS 165Ho(n, X), E=1.84 MeV; measured transmission; deduced 165Ho deformation σ. Rotating cryogenic aligned target.
doi: 10.1016/0168-9002(92)90825-O
1992KO21 Hyperfine Interactions 75, 165 (1992) J.E.Koster, E.D.Davis, C.R.Gould, D.G.Haase, N.R.Roberson, L.W.Seagondollar Test of Time Reversal Invariance in 2-MeV Neutron Scattering from Aligned 165Ho NUCLEAR REACTIONS 165Ho(polarized n, X), E=2 MeV; measured deformation effect, T-violating spin-flip asymmetry; deduced effective interaction parameter. Aligned target.
doi: 10.1007/BF02398973
1992PO13 Hyperfine Interactions 75, 153 (1992) H.Postma, J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.Knudson, G.E.Mitchell, S.Penttila, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Parity Violation at Neutron p-Wave Resonances of 238U and 232Th and Related Questions NUCLEAR REACTIONS 238U, 232Th(n, X), E ≈ epithermal; measured transmission. 239U, 233Th deduced p-wave resonances, parity violation matrix element rms value.
doi: 10.1007/BF02398972
1992SO01 Phys.Rev. C45, 326 (1992) J.P.Soderstrum, C.R.Gould, D.G.Haase, N.R.Roberson, M.B.Schneider, L.W.Seagondollar Transverse and Longitudinal Polarized-Neutron, Polarized-93Nb Scattering, and the Tensor Spin-Spin Potential NUCLEAR REACTIONS 93Nb(polarized n, n), E=7.5 MeV; measured spin-spin σ; deduced spin-spin potential parameters. Other data included. Cryogenically polarized target.
doi: 10.1103/PhysRevC.45.326
1992ZH12 Phys.Rev. C46, 768 (1992) X.Zhu, J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, and the TRIPLE Collaboration Parity Nonconservation for Neutron Resonances in 238U NUCLEAR REACTIONS 238U(polarized n, X), E=6-300 eV; measured total σ; deduced P-odd, P-even effective nucleon-nucleon interaction. 239U deduced resonances, l, gΓn, p-wave parity nonconserving matrix element rms value, spreading width.
doi: 10.1103/PhysRevC.46.768
1991FR08 Phys.Rev.Lett. 67, 564 (1991) C.M.Frankle, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, S.H.Yoo, V.W.Yuan, X.Zhu, and the TRIPLE Collaboration Sign Correlations and Parity Nonconservation for Neutron Resonances in 232Th NUCLEAR REACTIONS 232Th(polarized n, n), E ≈ 8.3-392 eV; measured longitudinal analyzing power vs E, transmission yield. 232Th resonances deduced parity violation evidence statistical significance. High confidence limit measurement.
doi: 10.1103/PhysRevLett.67.564
1991KO28 Phys.Lett. 267B, 23 (1991) J.E.Koster, E.D.Davis, C.R.Gould, D.G.Haase, N.R.Roberson, L.W.Seagondollar, S.Wilburn, X.Zhu Direct Reaction Test of T Violation in 2 MeV Neutron Scattering from Aligned 165Ho NUCLEAR REACTIONS 165Ho(polarized n, X), E=2 MeV; measured deformation effect, T-violating spin-flip asymmetries vs θ; deduced analyzing power, time reversal invariance validity, nucleon-nucleon interaction couplings T(odd)/T(even) ratio. Rotating, cryogenically-aligned target.
doi: 10.1016/0370-2693(91)90517-T
1991SZ05 Nucl.Phys. A527, 701c (1991) J.J.Szymanski, C.D.Bowman, J.D.Bowman, J.Knudson, S.Penttila, S.J.Seestrom, V.W.Yuan, J.E.Bush, C.M.Frankle, C.R.Gould, D.G.Haase, G.E.Mitchell, P.P.J.Delheij, H.Postma, N.R.Roberson, X.Zhu Parity and Time Reversal Symmetry Nonconservation in Neutron-Nucleus Interactions NUCLEAR REACTIONS 238U(polarized n, X), E=60-72 eV; measured transmission, resonance σ helicity dependence. 239U deduced p-, s-wave states mixing parity-violating rms matrix element, parity violating spreading width.
doi: 10.1016/0375-9474(91)90217-T
1991YU02 Phys.Rev. C44, 2187 (1991) V.W.Yuan, C.D.Bowman, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, X.Zhu Parity Nonconservation in Polarized-Neutron Transmission Through 139La NUCLEAR REACTIONS 139La(polarized n, X), E=0.5-1 eV; measured transmission. 140La resonance deduced asymmetry. Parity nonconservation, longitudinal beam polarization.
doi: 10.1103/PhysRevC.44.2187
1990BO26 Phys.Rev.Lett. 65, 1192 (1990) J.D.Bowman, C.D.Bowman, J.E.Bush, P.P.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.Knudson, G.E.Mitchell, S.Penttila, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.W.Yuan, X.Zhu Parity Nonconservation for Neutron Resonances in 238U NUCLEAR REACTIONS 238U(n, X), E=epithermal; measured transmission, σ(E) vs helicity. 239U levels deduced parity nonconservation.
doi: 10.1103/PhysRevLett.65.1192
1990PE19 J.Phys.(Paris), Colloq.C-6, 523 (1990) S.Penttila, C.D.Bowman, J.D.Bowman, J.E.Bush, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, H.Postma, N.R.Roberson, S.J.Seestrom, J.J.Szymanski, V.M.Yuan, X.Zhu Parity Violation in 239U Neutron Resonances NUCLEAR REACTIONS 238U(polarized n, X), E ≤ 250 eV; measured asymmetry in transmission; deduced parity violating matrix element rms value, effective NN-interaction parameter. 239U resonances deduced parity-violating spreading width.
1988HA40 Hyperfine Interactions 43, 133 (1988) D.G.Haase, C.R.Gould, J.E.Koster, N.R.Roberson, L.W.Seagondollar, J.P.Soderstrum, M.B.Schneider, X.Zhu Studies of Parity and Time Reversal Symmetries in Neutron Scattering from 165Ho NUCLEAR REACTIONS 165Ho(polarized n, X), E=7.1, 11 MeV; measured transmission differences; deduced parity, time violating analyzing powers.
doi: 10.1007/BF02398293
1988RA12 Nucl.Sci.Eng. 98, 348 (1988) P.Ramakrishnan, G.E.Mitchell, C.R.Gould, S.A.Wender, G.F.Auchampaugh Photon Production Cross Section for 181Ta NUCLEAR REACTIONS 181Ta(n, X), E=2-100 MeV; measured photon production σ(E, Eγ); deduced σ(E).
doi: 10.13182/NSE88-A23535
1988RA13 Nucl.Sci.Eng. 98, 357 (1988) P.Ramakrishnan, G.E.Mitchell, C.R.Gould, S.A.Wender, G.F.Auchampaugh, R.C.Little Neutron-Induced Photon Production Cross Sections NUCLEAR REACTIONS Ta(n, X), E < 20 MeV; measured Eγ, Iγ, photon production σ(E, Eγ); deduced σ(E).
doi: 10.13182/NSE88-A23536
1988SO10 Phys.Rev. C38, 2424 (1988) J.P.Soderstrum, C.R.Gould, D.G.Haase, L.W.Seagondollar, M.B.Schneider, N.R.Roberson Limits on P- and P, T-Violating Absorption of MeV Neutrons in 165Ho NUCLEAR REACTIONS 165Ho(polarized n, X), E=7.1, 11 MeV; measured P-violating analyzing power; deduced limits on P-, P-T violating absorption. Polarized neutron transmission through polarized, unpolarized targets.
doi: 10.1103/PhysRevC.38.2424
1986GO14 Radiat.Eff. 92, 139 (1986) C.R.Gould, J.Dave, G.E.Mitchell, P.Ramakrishnan, G.F.Auchampaugh, R.C.Little, S.A.Wender Photon Production Cross Section Measurements for Ta and Be NUCLEAR REACTIONS Ta, 9Be(n, γ), E=2-25 MeV; measured γ-ray production σ.
doi: 10.1080/00337578608208307
1986GO20 Phys.Rev.Lett. 57, 2371 (1986) C.R.Gould, D.G.Haase, L.W.Seagondollar, J.P.Soderstrum, K.E.Nash, M.B.Schneider, N.R.Roberson Spin-Spin Potentials in 27Al(pol) + n(pol) and the Nuclear Ramsauer Effect NUCLEAR REACTIONS 27Al(polarized n, n), E=5-17 MeV; measured spin-spin σ. Tof. Optical model.
doi: 10.1103/PhysRevLett.57.2371
1985TE01 Nucl.Sci.Eng. 91, 451 (1985) J.A.Templon, J.H.Dave, C.R.Gould, S.Singkarat Neutron Scattering Cross Sections from 14N and 9Be at 11, 14, and 17 MeV NUCLEAR REACTIONS 14N(n, n), 9Be(n, n), (n, n'), E=11, 14, 17 MeV; measured σ(θ); deduced optical model parameters, Coulomb correction terms.
doi: 10.13182/NSE85-A18361
1984WH01 Phys.Rev. C30, 1435 (1984) C.S.Whisnant, J.H.Dave, C.R.Gould Elastic and Inelastic Neutron Scattering from 27Al at 11, 14, and 17 MeV NUCLEAR REACTIONS 27Al(n, n), (n, n'), E=11, 14, 17 MeV; measured σ(θ); deduced spherical optical model, coupled-channel parameters.
doi: 10.1103/PhysRevC.30.1435
1983DA22 Phys.Rev. C28, 2212 (1983) Optical Model Analysis of Scattering of 7- to 15-MeV Neutrons from 1-p Shell Nuclei NUCLEAR REACTIONS 6,7Li, 9Be, 10,11B, 12,13C, 16O(n, n), E=7-15 MeV; measured σ(θ); deduced spherical optical model parameters.
doi: 10.1103/PhysRevC.28.2212
1982DA05 Nucl.Sci.Eng. 80, 388 (1982) J.H.Dave, C.R.Gould, L.W.Seagondollar, C.R.Howell, R.S.Pedroni, F.O.Purser, R.L.Walter Neutron Elastic and Inelastic Scattering Cross Sections for Carbon-13 between 10 and 18 MeV NUCLEAR REACTIONS 13C(n, n), (n, n'), E=10-18 MeV; measured σ(θ), σ(En). Legendre polynomial, optical model analyses.
doi: 10.13182/NSE82-A19823
1982DA21 Nucl.Instrum.Methods 200, 285 (1982) J.H.Dave, C.R.Gould, S.A.Wender, S.M.Shafroth The 1H(7Li, n)7Be Reaction as an Intense MeV Neutron Source NUCLEAR REACTIONS 1H(7Li, n), E=13.15-22 MeV; measured σ(θ) vs E. Tof.
doi: 10.1016/0167-5087(82)90444-6
1982EL09 Nucl.Phys. A390, 509 (1982) S.M.El-Kadi, C.E.Nelson, F.O.Purser, R.L.Walter, A.Beyerle, C.R.Gould, L.W.Seagondollar Elastic and Inelastic Scattering of Neutrons from 54,56Fe and 63,65Cu. (I). Measurements from 8 to 14 MeV and a Spherical Optical Model Analysis NUCLEAR REACTIONS 54,56Fe, 63,65Cu(n, n), (n, n'), E=8, 10, 12, 14 MeV; measured σ(θ); deduced new spherical optical potential parameters. Compared to earlier global potential parametrizations.
doi: 10.1016/0375-9474(82)90281-0
1982GL02 Nucl.Sci.Eng. 80, 256 (1982) S.G.Glendinning, S.El-Kadi, C.E.Nelson, R.S.Pedroni, F.O.Purser, R.L.Walter, A.G.Beyerle, C.R.Gould, L.W.Seagondollar, P.Thambidurai Elastic and Inelastic Neutron Cross Sections for Boron-10 and Boron-11 NUCLEAR REACTIONS 10B(n, n), E=8-14 MeV; 11B(n, n), (n, n'), E=8, 9, 9.7, 9.9, 11-14 MeV; measured σ(θ); deduced integrated σ(E). Legendre polynomial analysis.
doi: 10.13182/NSE82-A21429
1982GL09 Nucl.Sci.Eng. 82, 393 (1982) S.G.Glendinning, S.El-Kadi, C.E.Nelson, F.O.Purser, C.R.Gould, L.W.Seagondollar Neutron Elastic Scattering Cross Sections for 16O between 9 and 15 MeV NUCLEAR REACTIONS 16O(n, n), E=9.21-14.93 MeV; measured σ(θ), σ(En), σ(total) vs E. 17O deduced resonances, Γ, Γn, J, π. Optical model plus resonance effect, Legendre polynomial analyses.
doi: 10.13182/NSE82-A21453
1982TH07 Nucl.Instrum.Methods 196, 415 (1982) P.Thambidurai, A.G.Beyerle, C.R.Gould, F.O.Purser Tritium Break-Up Contribution to the Neutron Source Reaction 3H(p, n) from 9 to 14 MeV NUCLEAR REACTIONS 3H(p, n), E=9.77-14.77 MeV; measured σ(θ=0°) vs E; deduced σ(breakup). Neutron source reaction, tof.
doi: 10.1016/0029-554X(82)90106-9
1980CL03 Nucl.Phys. A339, 285 (1980) H.Clement, R.N.Boyd, C.R.Gould, T.B.Clegg Study of the Structure of the Low-Lying Levels of 29Si via the 28Si(d, pγ) Reaction and Multi-Step Reaction Calculations NUCLEAR REACTIONS 28Si(polarized d, pγ), E=7.6 MeV; measured pγ(θ). DWBA, CCBA calculations.
doi: 10.1016/0375-9474(80)90094-9
1980EY01 Phys.Rev. C21, 1377 (1980) Y.Eyal, A.Gavron, I.Tserruya, Z.Fraenkel, Y.Eisen, S.Wald, R.Bass, C.R.Gould, G.Kreyling, R.Renfordt, K.Stelzer, R.Zitzmann, A.Gobbi, U.Lynen, H.Stelzer, I.Rode, R.Bock Neutron Emission in Deep-Inelastic Collisions Induced by 86Kr on 166Er at 5.7, 7.0, and 7.9 MeV/Nucleon NUCLEAR REACTIONS 166Er(86Kr, X), E=496, 602, 675 MeV; measured n(fragment)(fragment)-, (fragment)(fragment)-coin; deduced σ(En), out-of-plane neutron anisotropy, multiplicities. Statistical model.
doi: 10.1103/PhysRevC.21.1377
1980GO04 Z.Phys. A294, 323 (1980) C.R.Gould, R.Bass, J.v.Czarnecki, V.Hartmann, K.Stelzer, R.Zitzmann, Y.Eyal Neutron Multiplicities in Inelastic Collisions of 132Xe with 197Au NUCLEAR REACTIONS 197Au(132Xe, X), E=990 MeV; measured (fragment)n-coin, En; deduced neutron multiplicities. Statistical model.
doi: 10.1007/BF01434140
1979HO11 Nucl.Sci.Eng. 69, 22 (1979) H.H.Hogue, P.L.von Behren, D.W.Glasgow, S.G.Glendinning, P.W.Lisowski, C.E.Nelson, F.O.Purser, W.Tornow, C.R.Gould, L.W.Seagondollar Elastic and Inelastic Scattering of 7- to 14-MeV Neutrons from Lithium-6 and Lithium-7 NUCLEAR REACTIONS 6,7Li(n, n), (n, n'), E=7-14 MeV; measured σ(θ), integral σ.
doi: 10.13182/NSE79-A21281
1978GO02 Z.Phys. A284, 353 (1978) C.R.Gould, R.Bass, J.v.Czarnecki, V.Hartmann, K.Stelzer, R.Zitzmann, Y.Eyal Neutron Multiplicities in Inelastic Collisions of 132Xe with 197Au NUCLEAR REACTIONS 197Au(132Xe, xn), E=7.5 MeV/amu; measured neutron multiplicities.
doi: 10.1007/BF01406809
1978HO23 Nucl.Sci.Eng. 68, 38 (1978) H.H.Hogue, P.L.Von Behren, D.H.Epperson, S.G.Glendinning, P.W.Lisowski, C.E.Nelson, H.W.Newson, F.O.Purser, W.Tornow, C.R.Gould, L.W.Seagondollar Differential Elastic and Inelastic Scattering of 7- to 15-MeV Neutrons from Beryllium NUCLEAR REACTIONS 9Be(n, n), (n, n'), E=7-15 MeV; measured σ(θ); deduced reaction mechanisms contributing to σ(n, 2n).
doi: 10.13182/NSE78-A27268
1978WE02 Phys.Rev. C17, 1260 (1978) H.R.Weller, R.A.Blue, P.L.Von Behren, N.R.Roberson, C.R.Gould, D.R.Tilley, S.A.Wender Angular Distribution Measurements for Radiative Capture of Fast Neutrons by 40Ca NUCLEAR REACTIONS 40Ca(n, γ), E=8.0, 12.0 MeV; measured σ(θ). DSD calculations.
doi: 10.1103/PhysRevC.17.1260
1978WE03 Phys.Rev. C17, 1365 (1978) S.A.Wender, C.R.Gould, D.R.Tilley, D.G.Rickel, R.W.Zurmuhle Confirmation of 8+ Assignment to the 11.86 MeV Level in 24Mg NUCLEAR REACTIONS 12C(16O, αγ), E=42 MeV; measured linear polarization, αγ-coin. 24Mg level deduced J, π.
doi: 10.1103/PhysRevC.17.1365
1977DI05 Nucl.Phys. A279, 430 (1977) T.R.Dittrich, C.R.Gould, G.E.Mitchell, E.G.Bilpuch, K.Stelzer High Resolution Proton Inelastic Scattering from 50Cr NUCLEAR REACTIONS 50Cr(p, p), (p, p'), E=2.00-3.03 MeV; measured σ(θ) at 24 p-wave resonances. 51Mn deduced J, π, Γp, Γp', magnitude, relative phase of inelastic decay amplitudes, S, proton strength functions.
doi: 10.1016/0375-9474(77)90577-2
1976GL11 Nucl.Sci.Eng. 61, 521 (1976) D.W.Glasgow, F.O.Purser, H.Hogue, J.C.Clement, K.Stelzer, G.Mack, J.R.Boyce, D.H.Epperson, S.G.Buccino, P.W.Lisowski, S.G.Glendinning, E.G.Bilpuch, H.W.Newson, C.R.Gould Differential Elastic and Inelastic Scattering of 9- to 15-MeV Neutrons From Carbon NUCLEAR REACTIONS 12C(n, n), (n, n'), E=9-15 MeV; measured σ(E, θ), absolute σ(E).
doi: 10.13182/NSE76-A14488
1976WE23 Phys.Rev. C14, 1179 (1976) S.A.Wender, C.R.Gould, D.R.Tilley, D.G.Rickel, J.D.Turner, N.R.Roberson g Factor of the 738 keV State in 43K NUCLEAR REACTIONS 40Ar(α, p), E=15 MeV; measured γγ(θ, H, t). 43K level deduced T1/2, g.
doi: 10.1103/PhysRevC.14.1179
1975DI13 Phys.Lett. 59B, 230 (1975) T.R.Dittrich, C.R.Gould, G.E.Mitchell, E.G.Bilpuch, K.Stelzer Channel Spin Mixing Ratios in High Resolution Proton Inelastic Scattering NUCLEAR REACTIONS 50Cr(p, p'γ), E=3 MeV; measured proton, γ(θ); deduced channel spin mixing.
doi: 10.1016/0370-2693(75)90033-7
1975WI05 Phys.Rev. C11, 1111 (1975) J.R.Williams, R.O.Nelson, C.R.Gould, D.R.Tilley Gamma Ray Linear Polarization Measurements for 29Al NUCLEAR REACTIONS 26Mg(α, p), E=11.26 MeV; measured linear polarization, pγ-coin. 29Al levels deduced J, π. Enriched target.
doi: 10.1103/PhysRevC.11.1111
1975WI28 Nucl.Phys. A253, 365 (1975) J.R.Williams, C.R.Gould, R.O.Nelson, D.R.Tilley, D.G.Rickel, N.R.Roberson A Study of the Low-Lying Levels in 61Ni NUCLEAR REACTIONS 58Fe(α, nγ), E=8 MeV; measured nγ-coin, γγ(θ), DSA, linear polarization. 60Ni(d, pγ), E=6 MeV; measured pγ-coin. 61Ni levels deduced J, π, δ, γ-branching, 3He. Enriched targets.
doi: 10.1016/0375-9474(75)90487-X
1974GO34 Nucl.Sci.Eng. 55, 267 (1974) C.R.Gould, R.O.Nelson, J.R.Williams, J.R.Boyce Cross-Section Requirements for Charged-Particle Fusion Reactors: The 6Li(p, 3He)α Reaction NUCLEAR REACTIONS 6Li(p, 3He), E=3-12 MeV; measured σ(E(3He), Eα, θ).
doi: 10.13182/NSE74-A23453
1974KE09 Nucl.Phys. A223, 253 (1974) W.Kessel, R.Bass, E.C.Hagen, N.R.Roberson, C.R.Gould, D.R.Tilley Study of Excited States of 39Ca and 39K NUCLEAR REACTIONS 36Ar(α, nγ), 36Ar(α, pγ), E=15.8, 17.0 MeV; measured Doppler-shift attenuation. 39Ca, 39K levels, deduced T1/2. Enriched 36Ar target.
doi: 10.1016/0375-9474(74)90413-8
1974NE08 Phys.Rev. C9, 2193 (1974) R.O.Nelson, C.R.Gould, D.R.Tilley, N.R.Robinson Mean Lifetimes of Levels in 59Cu NUCLEAR REACTIONS 58Ni(3He, dγ), E=11.6 MeV; measured Eγ, Iγ, dγ-coin, DSA. 59Cu deduced levels, T1/2, γ-branching, J, π.
doi: 10.1103/PhysRevC.9.2193
1973GO02 Phys.Rev.Lett. 30, 298 (1973) C.R.Gould, R.O.Nelson, J.R.Williams, D.R.Tilley, J.D.Hutton, N.R.Robertson, C.E.Busch, T.B.Clegg Application of Polarized Deuterons in (d, pγ) Angular Correlation Measurements NUCLEAR REACTIONS 12C, 30Si(d, pγ), E=4.15 MeV; measured pγ(θ). 13C, 31Si transitions deduced γ-mixing.
doi: 10.1103/PhysRevLett.30.298
1973GO10 Phys.Rev. C7, 1068 (1973); Erratum Phys.Rev. C8, 423 (1973) C.R.Gould, D.R.Tilley, N.R.Roberson Mean Lifetimes of Levels in 26Al NUCLEAR REACTIONS 24Mg(3He, pγ), E=6 MeV; measured σ(Ep, Eγ), Doppler shift attenuation. 26Al levels deduced T1/2.
doi: 10.1103/PhysRevC.7.1068
1973HU03 Nucl.Phys. A206, 403 (1973) J.D.Hutton, N.R.Roberson, C.R.Gould, D.R.Tilley A Study of Low-Lying Levels in 59Ni NUCLEAR REACTIONS 56Fe(α, nγ), E=8.5, 10.5 MeV; measured Doppler-shift attenuation, recoil distance, σ(Eα, Eγ, θ(αγ)). 59Ni levels deduced J, π, T1/2, γ-branching, γ-mixing. Enriched target.
doi: 10.1016/0375-9474(73)90543-5
1973NE18 Nucl.Phys. A215, 541 (1973) R.O.Nelson, C.R.Gould, D.R.Tilley, N.R.Roberson Study of Low-Lying Levels of 53Fe NUCLEAR REACTIONS 54Fe(p, d), E=29 MeV; measured σ(θ(d)). 50Cr(α, nγ), E=7.45, 8.7, 10.5; measured σ(θ(γ)), Doppler-shift attenuation. 53Fe deduced levels, L, S, T1/2, J, γ-mixing, B(M1), B(E2). Enriched targets.
doi: 10.1016/0375-9474(73)90487-9
1972BI06 Particles Nucl. 3, 105 (1972) High Resolution Search for the Jπ = 0+ T = 1 Level in 26Al Near 3.7 MeV NUCLEAR REACTIONS 24Mg(3He, pγ), E=6 MeV; measured σ(Ep, Eγ). 26Al deduced levels, decay modes, 3.75 MeV doublet.
1972GO02 Phys.Rev. C5, 281 (1972) C.R.Gould, N.R.Roberson, G.E.Mitchell, D.R.Tilley Properties of the 2.443- and 3.003-MeV Levels in 57Ni NUCLEAR REACTIONS 54Fe(α, n), E=9.2, 10.5 MeV; measured σ(θ(γ)), Doppler shift attenuation. 57Ni levels deduced J, π, T1/2.
doi: 10.1103/PhysRevC.5.281
1972HA22 Particles Nucl. 3, 92 (1972) E.C.Hagen, C.R.Gould, N.R.Roberson, D.R.Tilley Lifetime Measurements in 27Si NUCLEAR REACTIONS 24Mg(α, nγ), E=10.8, 12.61, 15.0 MeV; measured DSA, σ(En, Eγ). 27Si levels deduced T1/2, transition strengths.
1971RA03 Phys.Rev. C3, 1152 (1971) C.E.Ragan III, C.R.Gould, N.R.Roberson, G.E.Mitchell, D.R.Tilley Study of Low-Lying Levels of 37Ar NUCLEAR REACTIONS 34S(α, nγ), E=7.6-8.8 MeV; measured σ(E, Eγ, θ(γ)), Doppler shift attenuation. 37Ar deduced levels, T1/2, J, π.
doi: 10.1103/PhysRevC.3.1152
1971RA05 Phys.Rev. C3, 2076 (1971); Erratum Phys.Rev. C4, 2294 (1971) C.E.Ragan III, G.E.Mitchell, D.R.Tilley, C.R.Gould, N.R.Roberson Mean Lifetime of the 1.61 MeV Level in 37Ar NUCLEAR REACTIONS 34S(α, nγ), E=8.1 MeV; measured recoil distance. 37Ar level deduced T1/2.
doi: 10.1103/PhysRevC.3.2076
1970BA08 Phys.Rev. C1, 470 (1970) D.P.Balamuth, R.W.Zurmuhle, G.P.Anastassiou, C.R.Gould, C.M.Fou Alpha-Gamma Angular Correlations in the 40Ca(3He, αγ)39Ca Reaction NUCLEAR REACTIONS 40Ca(3He, αγ), E=12 MeV; measured σ(Eα, Eγ, θ(αγ)). 39Ca deduced levels, J, π, γ-mixing, γ-multipolarity.
doi: 10.1103/PhysRevC.1.470
1970GO18 Phys.Rev.Lett. 25, 463 (1970) C.R.Gould, E.C.Hagen, R.V.Poore, N.R.Roberson, G.E.Mitchell, D.R.Tilley Lifetimes of Low-Lying Levels in 57Ni NUCLEAR REACTIONS 54Fe(α, nγ), E=8.7, 9.2, 10.5 MeV; measured σ(E;En, Eγ), Doppler shift attenuation. 57Ni deduced levels, T1/2, B(λ).
doi: 10.1103/PhysRevLett.25.463
1970LA17 Nucl.Phys. A158, 43 (1970) G.P.Lamaze, C.R.Gould, C.E.Moss, N.R.Roberson, D.R.Tilley An Angular Correlation Study of the Low-Lying Levels of 29P NUCLEAR REACTIONS 32S(p, αγ), E=12.12, 12.89 MeV; measured σ(Eα, Eγ, θ(αγ)). 29P deduced levels, J, π, γ-branching ratios, γ-mixing ratios. Natural targets.
doi: 10.1016/0375-9474(70)90048-5
1970RA24 Phys.Rev. C2, 557 (1970) C.E.Ragan III, C.E.Moss, C.R.Gould, N.R.Roberson, G.E.Mitchell, D.R.Tilley Mean Lifetime of the 2.94-MeV Level in 33S NUCLEAR REACTIONS 30Si(α, nγ), E=7.8-8.4 MeV; measured σ(E, Eγ), recoil distance. 33S level deduced T1/2.
doi: 10.1103/PhysRevC.2.557
1969GO06 Phys.Rev. 188, 1792 (1969) C.R.Gould, D.P.Balamuth, P.F.Hinrichsen, R.W.Zurmuhle Particle-γ-Ray Angular-Correlation Study of 57Ni in the Reaction 58Ni(3He, αγ)57Ni NUCLEAR REACTIONS 58Ni(3He, αγ), E=15 MeV; measured σ(Eα, Eγ, θ(αγ)). 57Ni deduced levels, J, π, γ-multipolarities, γ-mixing, branching ratios.
doi: 10.1103/PhysRev.188.1792
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