NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = D.F.Measday Found 55 matches. 2007ME09 Phys.Rev. C 75, 045501 (2007) D.F.Measday, T.J.Stocki, H.Tam γ rays from muon capture in I, Au, and Bi NUCLEAR REACTIONS 127I(μ-, ν), (μ-, nν), (μ-, 2nν), (μ-, 3nν), (μ-, 4nν), (μ-, 5nν), (μ-, 6nν), E at rest; 197Au(μ-, nν), (μ-, 3nν), E at rest; 209Bi(μ-, nν), (μ-, 2nν), (μ-, 3nν), (μ-, 4nν), (μ-, 5nν), E at rest; measured Eγ, Iγ, X-ray spectra.
doi: 10.1103/PhysRevC.75.045501
2007ME18 Phys.Rev. C 76, 035504 (2007) D.F.Measday, T.J.Stocki, B.A.Moftah, H.Tam γ rays from muon capture in 27Al and natural Si NUCLEAR REACTIONS 27Al, 28Si(μ-, ν), (μ-, nν), (μ-, 2nν), (μ-, 3nν), (μ-, pν), (μ-, npν), E not given; measured Eγ, Iγ, yields.
doi: 10.1103/PhysRevC.76.035504
2006ME08 Phys.Rev. C 73, 045501 (2006) γ rays from muon capture in natural Ca, Fe, and Ni NUCLEAR REACTIONS Ca(μ-, νxnypzα)43K/41K/40K/39K/38K/37K/39Ar/38Ar/38Cl/37Cl/36Cl/35Cl/34Cl, E at rest; Fe(μ-, νxnypzα)56Mn/55Mn/54Mn/53Mn/54Cr, E at rest; Ni(μ-, νxnypzα)58Fe/56Fe/59Co/57Co, E at rest; measured Eγ, Iγ, yields.
doi: 10.1103/PhysRevC.73.045501
2002ST01 Nucl.Phys. A697, 55 (2002) T.J.Stocki, D.F.Measday, E.Gete, M.A.Saliba, B.A.Moftah, T.P.Gorringe Gamma Rays from Muon Capture in 14N NUCLEAR REACTIONS 14N(μ-, X)14C/13C/12C/10B, E=low; measured Eγ, Iγ; deduced yields. 13,14C deduced levels, transitions.
doi: 10.1016/S0375-9474(01)01249-0
2001BU05 Phys.Rev. C63, 034303 (2001) L.Buchmann, E.Gete, J.C.Chow, J.D.King, D.F.Measday β-Delayed Particle Decay of 9C and the A = 9, T = 1/2 Nuclear System: R-matrix fits, the A = 9 nuclear system, and the stellar reaction rate of 4He(αn, γ)9Be RADIOACTIVITY 9C(β+); analyzed β-spectra, β-delayed particle spectra, coincidences. 9B deduced levels, J, π, Gamow-Teller strengths. Multichannel, multistate R-matrix approach, astrophysical implications discussed. Shell model calculations.
doi: 10.1103/PhysRevC.63.034303
2001ME27 Phys.Rep. 354, 243 (2001) The Nuclear Physics of Muon Capture
doi: 10.1016/S0370-1573(01)00012-6
2001ST23 Phys.Rev. A64, 042505 (2001) T.J.Stocki, D.F.Measday, E.Gete, M.A.Saliba, J.Lange, T.P.Gorringe Hyperfine Transition in Light Muonic Atoms of Odd Z NUCLEAR REACTIONS 19F, Na, 27Al, P, Cl, K(μ-, nX), E at rest; measured neutron spectra, hyperfine transition rates. ATOMIC PHYSICS, Mesic-atoms 19F, Na, 27Al, P, Cl, K(μ-, nX), E at rest; measured neutron spectra, hyperfine transition rates.
doi: 10.1103/PhysRevA.64.042505
2000GE09 Phys.Rev. C61, 064310 (2000) E.Gete, L.Buchmann, R.E.Azuma, D.Anthony, N.Bateman, J.C.Chow, J.M.D'Auria, M.Dombsky, U.Giesen, C.Iliadis, K.P.Jackson, J.D.King, D.F.Measday, A.C.Morton β-Delayed Particle Decay of 9C and the A = 9, T = 1/2 Nuclear System: Experiment, data, and phenomenological analysis RADIOACTIVITY 9C(β+); measured Eβ, Iβ, β-delayed particle spectra, coincidences, angular correlations. 9B levels deduced excitation and decay branching ratios.
doi: 10.1103/PhysRevC.61.064310
1997GE12 Nucl.Instrum.Methods Phys.Res. A388, 212 (1997) E.Gete, D.F.Measday, B.A.Moftah, M.A.Saliba, T.J.Stocki Neutron-Induced Peaks in Ge Detectors from Evaporation Neutrons NUCLEAR REACTIONS Ge(n, n'), E ≈ 1-20 MeV; measured Eγ, Iγ; deduced no neutron energy lineshape dependence.
doi: 10.1016/S0168-9002(96)01163-1
1997MO11 Phys.Lett. 395B, 157 (1997) B.A.Moftah, E.Gete, D.F.Measday, D.S.Armstrong, J.Bauer, T.P.Gorringe, B.L.Johnson, B.Siebels, S.Stanislaus Muon Capture in 28Si and g(p)/g(a) NUCLEAR REACTIONS 28Si(μ-, ν), E at rest; measured νγ(θ); deduced angular correlation coefficient, g(p)/g(a).
doi: 10.1016/S0370-2693(97)00081-6
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.
1996JO21 Phys.Rev. C54, 2714 (1996) B.L.Johnson, T.P.Gorringe, D.S.Armstrong, J.Bauer, M.D.Hasinoff, M.A.Kovash, D.F.Measday, B.A.Moftah, R.Porter, D.H.Wright Observables in Muon Capture on 23Na and the Effective Weak Couplings g(∼)(a) and g(∼)(p) NUCLEAR REACTIONS 23Na(μ-, X), E at rest; measured γ spectra, yield after residuals decay. 23,22,21,20Ne, 20F levels deduced capture rates, hyperfine dependence.
doi: 10.1103/PhysRevC.54.2714
1994GO07 Phys.Rev.Lett. 72, 3472 (1994) T.P.Gorringe, B.L.Johnson, D.S.Armstrong, J.Bauer, M.A.Kovash, M.D.Hasinoff, D.F.Measday, B.A.Moftah, R.Porter, D.H.Wright Hyperfine Effect in μ- Capture on 23Na and g(p)/g(a) NUCLEAR REACTIONS 23Na(μ-, γ), E at rest; measured capture rates, hyperfine transition rate in Na metal; deduced (g(p)/g(a)). ATOMIC PHYSICS 23Na(μ-, γ), E at rest; measured capture rates, hyperfine transition rate in Na metal; deduced (g(p)/g(a)).
doi: 10.1103/PhysRevLett.72.3472
1994ST02 Phys.Rev.Lett. 72, 973 (1994) J.C.Stasko, B.Bassalleck, E.C.Booth, M.B.Chertok, D.Healey, R.Jacot-Guillarmod, M.A.Kovash, D.J.Mack, D.F.Measday, J.P.Miller, M.A.Moinester, D.Ottewell, M.A.Pickar, P.Weber Radiative Decay of the Δ Resonance: Analyzing powers for π-(p(pol)) → γn NUCLEAR REACTIONS 1H(π-, γ), E=100-250 MeV; measured radiative capture analyzing power vs θ, E. Polarized target.
doi: 10.1103/PhysRevLett.72.973
1993GO09 Phys.Lett. 309B, 241 (1993) T.P.Gorringe, B.L.Johnson, J.Bauer, M.A.Kovash, R.Porter, P.Gumplinger, M.D.Hasinoff, D.F.Measday, B.A.Moftah, D.S.Armstrong, D.H.Wright Measurement of Hyperfine Transition Rates in Muonic 19F, 23Na, 31P, and (nat)Cl NUCLEAR REACTIONS 19F, 23Na, Cl(μ-, ν), E at rest; measured capture transitions time spectra; deduced hyperfine transition rates. ATOMIC PHYSICS, Mesic-Atoms 19F, 23Na, Cl(μ-, ν), E at rest; measured capture transitions time spectra; deduced hyperfine transition rates.
doi: 10.1016/0370-2693(93)90927-A
1993GO27 Nucl.Instrum.Methods Phys.Res. B79, 303 (1993) T.P.Gorringe, J.Bauer, B.L.Johnson, M.A.Kovash, R.Porter, P.Gumplinger, M.D.Hasinoff, D.F.Measday, B.Moftah, D.S.Armstrong, D.H.Wright Measurement of the Hyperfine Transition Rates in μ- F, Na, Al, P, and Cl, and the Hyperfine Dependence of μ- Capture NUCLEAR MOMENTS 19F, 23Na, 27Al, 31P, 35,37Cl; measured hyperfine transition rates following muon capture.
doi: 10.1016/0168-583X(93)95350-E
1992ME12 Czech.J.Phys. B42, 1231 (1992) The Study of Hypernuclei via the (K-, π0) Reaction NUCLEAR REACTIONS 7Li(γ, K+), E at 1200 MeV/c; analyzed spectrum. 7Li(K-, π0), E not given; calculated spectrum; deduced 7He hypernucleus levels. Proposed high resolution experiment.
doi: 10.1007/BF01591402
1991ST09 Phys.Rev. C44, 2287 (1991) S.Stanislaus, D.Horvath, D.F.Measday, A.J.Noble, M.Salomon Total Cross Sections and Analyzing Powers for the Reaction p + p → p + p + π0 Near Threshold NUCLEAR REACTIONS 1H(polarized p, pπ0), E=320-500 MeV; measured pion spectra, σ(θ, π), total σ, analyzing powers; deduced pion production features.
doi: 10.1103/PhysRevC.44.2287
1990GA16 Phys.Rev. C42, R475 (1990) K.P.Gall, E.C.Booth, W.J.Fickinger, M.D.Hasinoff, N.P.Hessey, D.Horvath, J.Lowe, E.K.McIntyre, D.F.Measday, J.P.Miller, A.J.Noble, B.L.Roberts, D.K.Robinson, M.Sakitt, M.Salomon, D.A.Whitehouse Radiative Kaon Capture on Deuterium and the (Lambda)n Scattering Lengths NUCLEAR REACTIONS 2H(K-, γ), E at 680 MeV/c; measured Eγ, Iγ following capture; deduced (lambda)n-scattering length.
doi: 10.1103/PhysRevC.42.R475
1990HO15 Phys.Rev. A41, 5834 (1990) D.Horvath, K.A.Aniol, F.Entezami, D.F.Measday, A.J.Noble, S.Stanislaus, C.J.Virtue, A.S.Clough, D.F.Jackson, J.R.H.Smith, M.Salomon Experimental Study of Pion Capture by Hydrogen Bound in Molecules NUCLEAR REACTIONS 1H(π-, π0), (π-, γ), E at rest; measured σ(E(π)), Eγ, Iγ, En, γγ-coin; deduced pion capture probability. ATOMIC PHYSICS, Mesic-Atoms 1H(π-, π0), (π-, γ), E at rest; measured σ(E(π)), Eγ, Iγ, En, γγ-coin; deduced pion capture probability.
doi: 10.1103/PhysRevA.41.5834
1990ST06 Phys.Rev. C41, R1913 (1990) S.Stanislaus, D.Horvath, D.F.Measday, A.J.Noble, M.Salomon s-Wave Partial Cross Sections for the Reaction p + p → p + p + π0 NUCLEAR REACTIONS 1H(p, pπ0), E=320-500 MeV; measured σ(E); deduced s-wave contribution.
doi: 10.1103/PhysRevC.41.R1913
1989RO14 Nuovo Cim. 102A, 145 (1989) B.L.Roberts, E.C.Booth, K.P.Gall, E.K.McIntyre, J.P.Miller, D.A.Whitehouse, J.Lowe, N.P.Hessey, M.D.Hasinoff, D.F.Measday, A.J.Noble, C.E.Waltham, M.Sakitt, W.J.Fickinger, D.K.Robinson, D.Horvath, B.Bassalleck, J.R.Hall, K.D.Larson, D.M.Wolfe, A.L.Hallin, M.Salomon Radiative Hyperon Processes NUCLEAR REACTIONS 2H(K-, γ), E not given; analyzed γ-spectra. 1H(π-, γ), (K-, γ), E at rest; measured photon spectra.
doi: 10.1007/BF02735103
1989ST01 Phys.Rev. C39, 295 (1989) S.Stanislaus, D.S.Armstrong, D.F.Measday Search for the Spontaneous Emission of Pions RADIOACTIVITY Pb, 209Bi, 232Th, 238,235U, 252Cf; measured π0 production limit; deduced branching ratio limit relative to SF-decay.
doi: 10.1103/PhysRevC.39.295
1989ST03 Phys.Lett. 219B, 237 (1989) S.Stanislaus, D.S.Armstrong, D.F.Measday, P.Weber, M.Harston Search for T = 2 Dibaryons via π-d → γX NUCLEAR REACTIONS 2H(π-, X), E at rest; measured γ-yields; deduced no T=2 dibaryon evidence. ATOMIC PHYSICS, Mesic-Atoms 2H(π-, X), E at rest; measured γ-yields; deduced π-d mesic atom transition branching ratio limit.
doi: 10.1016/0370-2693(89)90384-5
1988BA40 Phys.Rev. C38, 875 (1988) A.Bagheri, K.A.Aniol, F.Entezami, M.D.Hasinoff, D.F.Measday, J.-M.Poutissou, M.Salomon, B.C.Robertson Reaction π-p → γn below the Δ Resonance NUCLEAR REACTIONS 1H(π-, γ), E=45.6-121.9 MeV; measured σ(θ), σ(E); deduced photomeson σ.
doi: 10.1103/PhysRevC.38.875
1988BA41 Phys.Rev. C38, 885 (1988) A.Bagheri, K.A.Aniol, F.Entezami, M.D.Hasinoff, D.F.Measday, J.-M.Poutissou, M.Salomon, B.C.Robertson Reaction π-p → π0n below the Δ Resonance NUCLEAR REACTIONS 1H(π-, π0), E=45.6-121.9 MeV; measured σ(θ), σ(E).
doi: 10.1103/PhysRevC.38.885
1987CO33 Nucl.Phys. A473, 747 (1987) F.Corriveau, M.D.Hasinoff, D.F.Measday, J.-M.Poutissou, M.Salomon The Panofsky Ratio in 3He NUCLEAR REACTIONS 3He(π-, π0), (π-, γ), E at rest; measured branching ratios.
doi: 10.1016/0375-9474(87)90278-8
1987ST28 Nucl.Phys. A475, 630 (1987) S.Stanislaus, F.Entezami, A.Bagheri, D.F.Measday, D.Garner Atomic Capture Ratios for Muons in Oxides ATOMIC PHYSICS, Mesic-Atoms 23Na, Mg, 27Al, Si, 31P, Ca, 45Sc, Ti, 50,51V, Cr, 55Mn, Fe, 59Co, Ni, Cu, Zn, 89Y, Zr, 93Nb, Mo, Ag, Cd, Sn, Sb, Te, Ba, Ce, Pr, Sm, Hg, Pb, 209Bi; measured negative muon capture ratios. Lifetime technique. Oxide targets.
doi: 10.1016/0375-9474(87)90229-6
1987ST29 Nucl.Phys. A475, 642 (1987) S.Stanislaus, F.Entezami, D.F.Measday Atomic Capture of Muons and Density ATOMIC PHYSICS, Mesic-Atoms Z=11-83; calculated atomic capture ratio vs density, Z.
doi: 10.1016/0375-9474(87)90230-2
1987SU06 Phys.Rev. C35, 2212 (1987) T.Suzuki, D.F.Measday, J.P.Roalsvig Total Nuclear Capture Rates for Negative Muons ATOMIC PHYSICS, Mesic-Atoms 6,7Li, 9Be, 10,11B, C, 13C, N, O, 18O, 19F, 23Na, Mg, 27Al, Si, P, S, Cl, K, Ca, Sc, Ti, V, Cr, Mn, Fe, 59Co, Ni, Cu, Zn, Ge, As, Se, Br, Sr, Zr, 93Nb, Mo, Ag, Cd, In, Sn, Sb, Te, I, Ba, Ce, Nd, Gd, Dy, Er, W, Au, Hg, Tl, Pb, Bi(μ-, γ), E=87 MeV/c; measured muonic atom T1/2; deduced total capture rates, hyperfine effects.
doi: 10.1103/PhysRevC.35.2212
1986LI02 Nucl.Phys. A449, 301 (1986) S.T.Lim, M.D.Hasinoff, D.F.Measday, T.J.Mulligan, K.Ebisawa A Study of the Reaction 28Si(p, γ)29P NUCLEAR REACTIONS, ICPND 28Si(p, γ), E=7-24 MeV; measured Eγ, Iγ, γ yield vs E, σ(Eγ, θ, E), γ(θ). 29P deduced levels, J, π, T, GDR, I(E2/E1). Isotopic target.
doi: 10.1016/0375-9474(86)90007-2
1984SA03 Nucl.Phys. A414, 493 (1984) M.Salomon, D.F.Measday, J.-M.Poutissou, B.C.Robertson Radiative Capture and Charge Exchange of Negative Pions on Protons at 26.4 and 39.3 MeV NUCLEAR REACTIONS 1H(π-, γ), (π-, π0), E=27.4, 39.3 MeV; measured σ(θ); deduced pion-nucleon phase shifts, scattering lengths.
doi: 10.1016/0375-9474(84)90615-8
1982ME03 Czech.J.Phys. B32, 138 (1982) Experiments on Pion Reactions below 50 MeV NUCLEAR REACTIONS 1H(π-, γ), (π-, π0), E=27.4, 39.3 MeV; measured Eγ, Iγ; deduced charge exchange scattering length. Liquid hydrogen target.
doi: 10.1007/BF01608040
1981BA16 Nucl.Phys. A362, 445 (1981) B.Bassalleck, F.Corriveau, M.D.Hasinoff, T.Marks, D.F.Measday, J.-M.Poutissou, M.Salomon The Observation of Charge Exchange of Pions Captured in Several Nuclei NUCLEAR REACTIONS 6Li, Al, Ti, Cu, Nb, Pb(π-, π0), E at rest; measured branching ratios. 6Li deduced Panofsky ratio.
doi: 10.1016/0375-9474(81)90504-2
1981HI05 Nucl.Phys. A365, 333 (1981) V.L.Highland, M.Salomon, M.D.Hasinoff, E.Mazzucato, D.F.Measday, J.-M.Poutissou, T.Suzuki Branching Ratios for Stopped Pions in Deuterium NUCLEAR REACTIONS 2H(π-, n), (π-, nγ), E at rest; measured branching ratio.
doi: 10.1016/0375-9474(81)90395-X
1980SU03 Phys.Lett. B95, 202 (1980) T.Suzuki, R.J.Mikula, D.M.Garner, D.G.Fleming, D.F.Measday Muon Capture in Oxides Using the Lifetime Method NUCLEAR REACTIONS C, Na, Mg, Al, Si, P, Ca, Ti, Cr, Mn, Cu, Zn, Ge, Cd, Sn, Ba, Nd, Hg, Pb(μ-, e), E at rest; measured relative muon capture rate. Oxide targets, lifetime method.
doi: 10.1016/0370-2693(80)90469-4
1979SC07 Nucl.Phys. A316, 317 (1979) P.Schwaller, M.Pepin, B.Favier, C.Richard-Serre, D.F.Measday, P.U.Renberg Proton Total Cross Sections on 1H, 2H, 4He, 9Be, C and O in the Energy Range 180 to 560 MeV NUCLEAR REACTIONS 1,2H, 4He, 9Be, C, O(p, X), E=180-560 MeV; measured σ(E). Enriched, natural targets. Glauber model calculations.
doi: 10.1016/0375-9474(79)90040-X
1977MA08 Phys.Rev.Lett. 38, 746 (1977) R.MacDonald, D.S.Beder, D.Berghofer, M.D.Hasinoff, D.F.Measday, M.Salomon, J.Sputter, T.Suzuki, J.M.Poutissou, R.Poutissou, P.Depommier, J.K.P.Lee Charge Exchange of Stopped π- in Deuterium: Experiment and Theory NUCLEAR REACTIONS 2H(π-, π0), (π-, X), E ≈ 0 MeV; measured spectra; deduced reaction branching.
doi: 10.1103/PhysRevLett.38.746
1976BE28 Nucl.Phys. A263, 109 (1976) D.Berghofer, M.D.Hasinoff, R.Helmer, S.T.Lim, D.F.Measday, K.Ebisawa High-Energy Levels in 13N (II) NUCLEAR REACTIONS 12C(p, γ), (p, p'γ), E=9-24 MeV; measured σ(Ep, θ). 13N deduced resonances. Enriched target.
doi: 10.1016/0375-9474(76)90187-1
1975SP04 Nucl.Phys. A248, 276 (1975) J.Spuller, M.D.Hasinoff, S.T.Lim, D.F.Measday, T.J.Mulligan Isospin Violation in α-Induced Reactions NUCLEAR REACTIONS 12C(α, α'γ), (α, pγ), 10B(α, dγ), E=18-27 MeV; measured σ(E, Eγ). 16O levels deduced isospin mixing. Enriched targets.
doi: 10.1016/0375-9474(75)90166-9
1973ME12 Can.J.Phys. 51, 1227 (1973) D.F.Measday, M.Hasinoff, D.L.Johnson High-Energy Levels in 13N NUCLEAR REACTIONS 12C(p, γ), (p, p'γ), E=9-24 MeV; measured Eγ, Iγ. 13N deduced resonances, level-width. 12C deduced levels, π.
doi: 10.1139/p73-160
1972HA32 Phys.Lett. 39B, 506 (1972) M.Hasinoff, D.Johnson, D.F.Measday Destructive Interference in Radiative Proton Capture Reactions NUCLEAR REACTIONS 12C(p, γ), E=8.6-16.3 MeV; measured σ(E); deduced destructive interference. 13N deduced resonances, level-width.
doi: 10.1016/0370-2693(72)90331-0
1972RE06 Nucl.Phys. A183, 81 (1972) P.U.Renberg, D.F.Measday, M.Pepin, P.Schwaller, B.Favier, C.Richard-Serre Reaction Cross Sections for Protons in the Energy Range 220-570 MeV NUCLEAR REACTIONS Be, C, Al, Fe, Cu, Ge, Sn, Pb(p, X), E=220-570 MeV; measured σ(E); H, B, O, Na deduced σ(E).
doi: 10.1016/0375-9474(72)90932-3
1967ME07 Phys.Letters 25B, 106 (1967) Unbound Energy Levels in 4H NUCLEAR REACTIONS 4He(n, p), E=152 MeV; measured proton spectra. 4H deduced possible unbound level.
doi: 10.1016/0370-2693(67)90192-X
1967ME11 Phys.Rev. 161, 1071 (1967) (n, p) and (n, d) Reactions at 152 MeV NUCLEAR STRUCTURE 51Ti, 40K, 12C, 9Be, 7Li, 6Li, 27Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.161.1071
1966ME01 Nucl.Phys. 78, 476(1966) The 12C(p, pn)11C Reaction from 5.0 to 160 MeV NUCLEAR REACTIONS 12C(p, pn), E=50-160 MeV; measured σ(E). Natural target.
doi: 10.1016/0029-5582(66)90621-3
1966ME03 Phys.Letters 21, 62 (1966) A Study of the (n, d) Reaction at 152 MeV NUCLEAR STRUCTURE 12C, 7Li, 6Li, 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91342-4
1966ME04 Phys.Letters 21, 66 (1966) The 2H(n, p)2n reaction at 152 MeV NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91344-8
1966ME14 Nucl.Phys. 85, 129(1966) Neutron Total Cross Sections in the Energy Range 80 to 150 MeV NUCLEAR REACTIONS 4He, 12C, 14N, 16O, 27Al(n, X), E = 80-150 MeV; measured σ(nT)(E). Natural targets.
doi: 10.1016/0029-5582(66)90136-2
1966ME15 Nucl.Phys. 85, 142(1966) Neutron Total Cross Sections for Neutrons, Protons and Deuterons in the Energy Range of 90 to 150 MeV NUCLEAR REACTIONS 1H(n, X), 2H(n, X), E = 80-150 MeV; measured σ(E). 1n, 2H(n, n); deduced σ(E). Natural, enriched targets.
doi: 10.1016/0029-5582(66)90137-4
1966ME21 Phys.Rev. 142, 584 (1966) Neutron-Proton Differential Cross Section At 129 And 150 Mev NUCLEAR REACTIONS 1H(n, n), E=129-150 MeV; measured products, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry 11123.
doi: 10.1103/PhysRev.142.584
1964ME09 Bull.Am.Phys.Soc. 9, No.7, 724, O4 (1964) Total Neutron Cross Sections from 90 to 150 MeV NUCLEAR STRUCTURE Al, O, C, N; measured not abstracted; deduced nuclear properties.
1963FI07 Nucl.Phys. 45, 113 (1963) P.S.Fisher, D.F.Measday, F.A.Nikolaev, A.Kalmykov, A.B.Clegg The C12(p, γ) Reaction from 10 to 50 MeV NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90787-9
1963ME04 Nucl.Phys. 45, 98 (1963) D.F.Measday, P.S.Fisher, A.Kalmykov, F.A.Nikolaev, A.B.Clegg The C12(p, p')C12*(12.71 and 15.11 Mev) Reaction from Threshold to 50 MeV NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90786-7
1962ME05 Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 11, 4.3 (September 1962) D.F.Measday, P.S.Fisher, A.Kalmykov, F.A.Nikolaev, A.B.Clegg NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
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