NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = R.H.Pehl Found 32 matches. 1997HU16 Nucl.Instrum.Methods Phys.Res. A385, 489 (1997) E.L.Hull, R.H.Pehl, M.R.Stanley, C.C.Foster, K.Komisarcik, G.W.East, J.D.Vanderwerp, D.L.Friesel A 16N Gamma-Ray Facility RADIOACTIVITY 16N(β-) [from 16O(n, p)]; measured Eγ, Iγ. Gamma-ray source for detector calibration.
doi: 10.1016/S0168-9002(96)01028-5
1996PE30 Nucl.Instrum.Methods Phys.Res. A381, 97 (1996) R.H.Pehl, E.L.Hull, N.W.Madden, J.Xing, D.L.Friesel Gamma-Ray Escape Peak Characteristics of Radiation-Damaged Reverse-Electrode Germanium Coaxial Detectors RADIOACTIVITY 60Co(β-); measured Eγ, Iγ; deduced response vs position in radiation-damaged coaxial Ge detectors.
doi: 10.1016/0168-9002(96)00648-1
1986CA07 Phys.Rev. D33, 2737 (1986) D.O.Caldwell, R.M.Eisberg, D.M.Grumm, D.L.Hale, M.S.Witherell, F.S.Goulding, D.A.Landis, N.W.Madden, D.F.Malone, R.H.Pehl, A.R.Smith Half-Life Limits on the Zero-Neutrino and Two-Neutrino Double-β Decay of 76Ge RADIOACTIVITY 76Ge(2β); measured zero-, two-neutrino double β-decay T1/2 lower limit.
doi: 10.1103/PhysRevD.33.2737
1983FR10 Nucl.Instrum.Methods 207, 403 (1983) D.L.Friesel, B.S.Flanders, R.H.Pehl A Variable Geometry High-Purity Germanium Detector Telescope System for use with Intermediate Energy Charged Particles NUCLEAR REACTIONS 62Ni(p, p'), (p, d), (p, t), E=60 MeV; 28Si(p, p'), E=115 MeV; 12C(3He, t), E=200 MeV; measured σ(Ep'), σ(Ed), σ(Et); 40Ca(p, 2p), E=150 MeV; measured pp-coin. Variable geometry telescope detector system.
doi: 10.1016/0167-5087(83)90651-8
1982DO01 Phys.Rev. C25, 962 (1982) K.G.R.Doss, P.D.Barnes, N.Colella, S.A.Dytman, R.A.Eisenstein, C.Ellegaard, F.Takeutchi, W.R.Wharton, J.F.Amann, R.H.Pehl, A.C.Thompson (π+, p) and (π+, d) Reactions on Light Nuclei NUCLEAR REACTIONS 12,13C, 16O(π+, p), (π+, d), 7Li, 10B, 18O(π+, d), E=32-81 MeV; measured σ(Ep), σ(Ed), σ(θ). 8B, 10,11C, 14,16O levels deduced L, relative two-nucleon pickup strength. High purity Ge detectors. Betz-Kerman model.
doi: 10.1103/PhysRevC.25.962
1974TH06 Nucl.Instrum.Methods 121, 65 (1974) Characteristics of a High-Purity Germanium Detector NUCLEAR REACTIONS 14N(n, γ); measured Eγ, Iγ. 15N deduced transitions.
doi: 10.1016/0029-554X(74)90140-2
1966CE01 Phys.Rev.Letters 16, 469 (1966) J.Cerny, S.W.Cosper, G.W.Butler, R.H.Pehl, F.S.Goulding, D.A.Landis, C.Detraz Mass of 3He from the Four-Neutron Transfer Reaction 26Mg(α, 8He)22Mg NUCLEAR STRUCTURE 8He, 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.16.469
1966CE02 Phys.Letters 20, 35 (1966) J.Cerny, R.H.Pehl, G.Butler, D.G.Fleming, C.Maples, C.Detraz The Mass 13, T = 3/2 Quartet NUCLEAR STRUCTURE 13O, 13N, 15N, 13C, 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91037-7
1966CE05 Phys.Rev. 152, 950 (1966) Study of Mass 5 and 7 Nuclei by (p, t) and (p, 3He) Reactions on 7Li and 9Be NUCLEAR STRUCTURE 5He, 5Li, 7Be, 9Be, 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.152.950
1966RI04 Phys.Rev. 141, 1021 (1966) E.Rivet, R.H.Pehl, J.Cerny, B.G.Harvey Investigation of High Spin Levels Preferentially Populated by the (α, d) Reaction NUCLEAR STRUCTURE 14N, 16O, 26Al, 28Al, 12C, 30P, 42K, 42Sc, 18F, 22Na, 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.141.1021
1965CE02 Phys.Rev.Lett. 15, 300 (1965) Li4 and the Excited Levels of He4 NUCLEAR REACTIONS 6Li(p, t), (p, 3He), 7Li(p, α), E=43.7 MeV; measured reaction products. 4Li, 4He; deduced partial σ(θ) for excited states, level energies, J, π. Comparison with available data. Berkeley 88-in. cyclotron.
doi: 10.1103/PhysRevLett.15.300
1965CE03 UCRL-16580, p.61 (1965) Li4 and the Excited Levels of He4 NUCLEAR STRUCTURE 6Li, 7Li; measured not abstracted; deduced nuclear properties.
1965DE08 Phys.Rev.Letters 14, 708 (1965) Observation of T=3/2 Levels in Li7 -Be7 and the Uncharacterized Nuclei He7, B7, and He8 NUCLEAR STRUCTURE 9Be, 7He, 7B, 8He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.14.708
1965PE03 Phys.Rev. 137, B114 (1965) R.H.Pehl, E.Rivet, J.Cerny, B.G.Harvey C12(α, d)N14 Reaction NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.137.B114
1965PE04 Phys.Letters 14, 137 (1965) Corrected Na20 Mass and Levels in Na20 and F16 Using the (He3, t) Reaction NUCLEAR STRUCTURE 20Ne, 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90454-3
1965PE17 Phys.Rev. 140, B605 (1965) R.H.Pehl, J.Cerny, E.Rivet, B.G.Harvey (d, α) Reactions on C12, N14, and O16 Induced by 24-MeV Deuterons NUCLEAR STRUCTURE 16O, 14N, 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B605
1964CE02 Phys. Rev. Letters 12, 619 (1964) Comparison of the 16O(p, t) and (p, 3He) Reactions Populating Analog Final States in 14O and 14N NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.12.619
1964CE03 Bull. Am. Phys. Soc. 9, No. 7, 704, B10 (1964) J.Cerny, R.H.Pehl, D.G.Fleming, C.C.Maples Observation of T=3/2 States in C13 and N13 via (p, He3) and (p, t) Reactions on N15 NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.
1964CE04 Phys. Rev. Letters 13, 726 (1964) J.Cerny, R.H.Pehl, F.S.Goulding, D.A.Landis Completion of the Mass-9 Isobaric Quartet via the Three-Neutron Pickup Reaction C12(He3, He6)C9 NUCLEAR STRUCTURE 9C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.13.726
1964CE05 Phys. Letters 12, 234 (1964) T=2 States in the T(Z)=0 Nuclei O16-Ne20 and the T(Z)=1 Nuclei N16-F20
doi: 10.1103/PhysRevLett.12.619
1964GA02 Phys.Rev.Letters 12, 726 (1964) T = 2 States in Mg24, Ti44, and Fe52 NUCLEAR STRUCTURE 24Mg, 44Ti, 52Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.12.726
1964RI03 UCRL-11213, p.71 (1964) E.J-M.Rivet, J.Cerny, B.G.Harvey, R.H.Pehl, J.Haag The Formation of Strongly Populated High Spin Levels in (α, d) Reactions NUCLEAR STRUCTURE 42K, 42Sc, 26Al, 22Na; measured not abstracted; deduced nuclear properties.
1963CE02 Phys.Letters 7, 67 (1963) J.Cerny, R.H.Pehl, E.Rivet, B.G.Harvey Investigation of Isobaric-Spin Conservation in the O16(d, α)N14 Reaction Using a High Resolution Semiconductor E-(dE/dx) System NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90445-1
1962CE01 Nuclear Phys. 29, 120 (1962) (α, d) Reactions on Odd Targets NUCLEAR STRUCTURE 6Li, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90171-2
1962HA40 Nuclear Phys. 39, 160 (1962) B.G.Harvey, J.Cerny, R.H.Pehl, E.Rivet Levels Involving A (d5/2)52 State in Light Nuclei
doi: 10.1016/0029-5582(62)90383-8
1962HA48 UCRL-10624, p.181 (1962) B.G.Harvey, J.Cerny, R.H.Pehl, E.J.M.Rivet Two-Nucleon Stripping Reactions NUCLEAR STRUCTURE 42Sc, 42K; measured not abstracted; deduced nuclear properties.
1962WI19 UCRL-10624, p.159 (1962) B.D.Wilkins, R.H.Pehl, N.K.Glendenning Optical-Model Analysis for 10-MeV Protons
1961CE02 Bull.Am.Phys.Soc. 6, No.6, 507, E11 (1961) J.Cerny, N.K.Glendenning, B.G.Harvey, R.H.Pehl, E.Rivet Analysis of the Two-Nucleon Stripping Reaction C12(He3, p)N14 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1961PE24 UCRL-10023, p.121 (1961) Investigation of Isobaric-Spin Conservation in the O16(d, α)N14 Reaction using a High-Resolution Semiconductor E-dE/dx System
1961RI07 UCRL-10023, p.117 (1961) E.Rivet, J.Cerny, B.C.Harvey, R.H.Pehl A Two-Nucleon Stripping Analysis of the C12(He3, p)N14 Reaction NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1960CE01 Bull.Am.Phys.Soc. 5, No.7, 493, C3 (1960) Reactions Li6(α, d)Be8 and Li7(α, d)Be9 with 48-MeV Helium Ions NUCLEAR STRUCTURE 9Be, 8Be; measured not abstracted; deduced nuclear properties.
1960HA31 Bull.Am.Phys.Soc. 5, No.7, 493, C4 (1960) Comparison of the Reactions C12(He3, n)N14 and C12(α, d)N14 NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
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