NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = N.Jarmie Found 66 matches. 1990BR04 Phys.Rev. C41, 1391 (1990) Differential Cross Sections at Low Energies for 2H(d, p)3H and 2H(d, n)3He NUCLEAR REACTIONS, ICPND 2H(d, n), (d, p), E=20-117 keV; measured σ(E, θ); deduced σ(E), astrophysical S-factor vs E. Analytical, R-matrix fits.
doi: 10.1103/PhysRevC.41.1391
1987BR10 Phys.Rev. C35, 1999 (1987); Erratum Phys.Rev. C36, 1220 (1987) Fusion-Energy Reaction 3H(d, α)n at Low Energies NUCLEAR REACTIONS, ICPND 3H(d, α), E=80-116 keV; measured σ(E); deduced astrophysical S-factor vs E. 5He deduced resonances, Γα, Γd. Flowing gas target, Si surface barrier detectors.
doi: 10.1103/PhysRevC.35.1999
1987CO34 Nucl.Phys. A475, 407 (1987) F.D.Correll, R.E.Brown, G.G.Ohlsen, R.A.Hardekopf, N.Jarmie, J.M.Lambert, P.A.Treado, I.Slaus, P.Schwandt, P.Doleschall Study of the Reaction H(d(pol), 2p)n at 16 MeV Around Collinear Configurations NUCLEAR REACTIONS, MECPD 1H(polarized d, 2p), E=16 MeV; measured σ(E(p3), θ(p3), E(p4), θ(p4)), analyzing powers vs arc length. Three-body Faddeev analysis.
doi: 10.1016/0375-9474(87)90071-6
1987HA20 Phys.Rev.Lett. 59, 763 (1987) Pole Structure of the J(π) = (3/2)+ Resonance in 5He NUCLEAR REACTIONS 3H(d, d), E(cm) ≤ 100 keV; calculated S-matrix amplitudes; deduced S-matrix poles. 5He deduced resonance, parameters Γ, Γn, Γd. R-matrix.
doi: 10.1103/PhysRevLett.59.763
1987HA44 Phys.Rev.Lett. 59, 2819 (1987) Hale, Brown, and Jarmie Reply:
doi: 10.1103/PhysRevLett.59.2819
1986BR20 Radiat.Eff. 92, 45 (1986) Hydrogen Fusion-Energy Reactions NUCLEAR REACTIONS, ICPND 2H(t, α), E=12.5-117 keV; measured σ; deduced astrophysical S-factor vs E. 2H(d, n), (d, p), E ≤ 125 keV; measured S-factor, anisotropy vs E. 3H(t, α), E ≤ 120 keV; measured σ(Eα); deduced astrophysical S-factor vs E.
doi: 10.1080/00337578608208295
1986MO05 Phys.Rev. C33, 1224 (1986) G.L.Morgan, P.W.Lisowski, S.A.Wender, R.E.Brown, N.Jarmie, J.F.Wilkerson, D.M.Drake Measurement of the Branching Ratio 3H(d, γ)/3H(d, n) using Thick Tritium Gas Targets NUCLEAR REACTIONS, ICPND 3H(d, γ), (d, n), E=0.0-0.72 MeV; measured Eγ, Iγ, En, relative γ yield. 5He resonance deduced branching ratio.
doi: 10.1103/PhysRevC.33.1224
1985BR33 Nucl.Instrum.Methods Phys.Res. B10/11, 356 (1985) R.E.Brown, R.A.Hardekopf, N.Jarmie, F.D.Correll, J.M.Lambert, P.A.Treado, I.Slaus, P.Schwandt, W.W.Jacobs, H.O.Meyer, E.J.Stephenson, J.Q.Yang, W.T.H.van Oers, P.Doleschall, J.A.Tjon Polarization in Three-Nucleon Breakup: Experiment and theory NUCLEAR REACTIONS 1H(polarized d, d), E=16, 79 MeV; measured vector analyzing power vs rotation angle. Faddeev formalism.
doi: 10.1016/0168-583X(85)90268-X
1985CE13 Phys.Rev. C32, 690 (1985) F.E.Cecil, D.M.Cole, R.Philbin, N.Jarmie, R.E.Brown Reaction 2H(3He, γ)5Li at Center-of-Mass Energies between 25 and 60 keV NUCLEAR REACTIONS, ICPND 2H(3He, γ), E(cm)=25-60 keV; measured Eγ, Iγ; deduced relative σ. 2H(3He, p), E=140 keV; measured σ(Ep), σ(Eα); deduced Γγ/Γp, relative σ. 5Li deduced level energy, relative γ-branching ratio. 4He level deduced γ-branching ratios.
doi: 10.1103/PhysRevC.32.690
1985JA16 Nucl.Instrum.Methods Phys.Res. B10/11, 405 (1985) Low-Energy Nuclear Reactions with Hydrogen Isotopes NUCLEAR REACTIONS, ICPND 2H(d, p), (d, 3He), E=20-117 keV; measured σ; deduced σ(E) for 2H(d, 3He), astrophysical S-function vs E.
doi: 10.1016/0168-583X(85)90279-4
1984JA08 Phys.Rev. C29, 2031 (1984); Erratum Phys.Rev. C33, 385 (1986) N.Jarmie, R.E.Brown, R.A.Hardekopf Fusion-Energy Reaction 2H(t, α)n from E(t) = 12.5 to 117 keV NUCLEAR REACTIONS, ICPND 2H(t, α), E=12.5-117 keV; measured fusion σ(E), σ(Eα), astrophysical S-function vs E; deduced Maxwellian reactivities upto plasma temperatures. Single level R-matrix analysis. 2H(p, p), E=10.04 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.29.2031
1983CE01 Phys.Rev. C27, 6 (1983) F.E.Cecil, R.F.Fahlsing, N.Jarmie, R.A.Hardekopf, R.Martinez Low-Energy 7Li(t, α)6He Cross Sections NUCLEAR REACTIONS 7Li, 9Be, 11B(t, α), E=70-110 keV; measured thick target yields; deduced σ(θ, E), astrophyscial S-factor vs θ, E.
doi: 10.1103/PhysRevC.27.6
1983GA03 Phys.Rev. C27, 1353 (1983) C.A.Gagliardi, G.T.Garvey, N.Jarmie, R.G.H.Robertson 0+ → 0- Beta Decay of 16C RADIOACTIVITY 16C(β-), (β-n) [from 14C(t, p), E=6 MeV]; measured β(t), γ(t), βγ-coin; deduced log ft. 16N levels deduced β-branching ratio.
doi: 10.1103/PhysRevC.27.1353
1983RO01 Phys.Rev. C27, 11 (1983) R.G.H.Roberston, P.Dyer, T.J.Bowles, R.E.Brown, N.Jarmie, C.J.Maggiore, S.M.Austin Cross Section of the Capture Reaction 3He(α, γ)7Be NUCLEAR REACTIONS, ICPND 3He(α, γ), 4He(3He, γ), E(cm)=897 keV; measured σ; deduced astrophysical capture σ. Activation technique.
doi: 10.1103/PhysRevC.27.11
1983SL01 Nucl.Phys. A397, 205 (1983) I.Slaus, J.M.Lambert, P.A.Treado, F.D.Correll, R.E.Brown, R.A.Hardekopf, N.Jarmie, Y.Koike, W.Gruebler The 4He(d(pol), αp)n Reaction at 12 and 17 MeV NUCLEAR REACTIONS 4He(polarized d, pα), E=12, 17 MeV; measured σ(E(α), θ(α), E(p), θ(p)), analyzing powers vs arc length. Three-body Fadeev analysis, energy and angle dependence.
doi: 10.1016/0375-9474(83)90102-1
1982BA45 Nucl.Phys. A388, 542 (1982) J.M.Barnwell, R.J.Griffiths, R.E.Brown, R.A.Hardekopf, N.Jarmie, F.D.Correll The Interactions of Polarised Tritons with 32S NUCLEAR REACTIONS 32S(polarized t, t), (polarized t, t'), (polarized t, α), E=17 MeV; measured σ(θ), A(θ). 31P levels deduced spectroscopic factors. Optical model, DWBA, CCBA analyses.
doi: 10.1016/0375-9474(82)90476-6
1981CO07 Phys.Rev. C23, 960 (1981) F.D.Correll, G.G.Ohlsen, R.E.Brown, R.A.Hardekopf, N.Jarmie, P.Doleschall Kinematically Incomplete Three-Nucleon Breakup Reaction 1H(pol(d), p)pn at 16 MeV NUCLEAR REACTIONS 1H(polarized d, p), E=16 MeV; measured analyzing power vs Ep, θ. Kinematically incomplete breakup reaction, Faddeev calculation.
doi: 10.1103/PhysRevC.23.960
1979AN15 Phys.Rev. C20, 897 (1979) B.D.Anderson, N.Jarmie, R.J.Barrett, E.D.Arthur The 16O(d, p)17O Reaction to the Unbound 5.09-MeV State of 17O NUCLEAR REACTIONS 16O(d, d), (d, p), E=12 MeV; measured σ(θ). 17O level deduced Γn. DWBA calculations for unbound states.
doi: 10.1103/PhysRevC.20.897
1979BR18 Phys.Rev. C20, 892 (1979) R.E.Brown, F.D.Correll, R.F.Haglund, Jr., R.A.Hardekopf, N.Jarmie, G.G.Ohlsen, P.A.Schmelzbach Direct-Reaction and Isospin Symmetries in d + d Reactions NUCLEAR REACTIONS 2H(polarized d, p), E=13.39, 15.50, 17.00 MeV; 2H(polarized d, n), E=15.50, 17.00 MeV; measured analyzing power(θ).
doi: 10.1103/PhysRevC.20.892
1979GR13 Nucl.Phys. A331, 61 (1979) W.Gruebler, R.E.Brown, F.D.Correll, R.A.Hardekopf, N.Jarmie, G.G.Ohlsen d + α Scattering from 12 to 17 MeV NUCLEAR REACTIONS 4He(polarized d, d), E=12, 14, 15, 17 MeV; measured σ(θ), vector, tensor analyzing power, A(θ). Phase-shift analysis.
doi: 10.1016/0375-9474(79)90301-4
1978HA38 Phys.Lett. 79B, 35 (1978) R.F.Haglund, Jr., R.E.Brown, N.Jarmie, G.G.Ohlsen, P.A.Schmelzbach, D.Fick Triton-Proton Elastic Scattering and Spin-Dependent Nucleon-Nucleon Forces NUCLEAR REACTIONS 1H(polarized t, t), E(cm)=1.26-3.71 MeV; measured σ(θ), analyzing power A(Et, θ).
doi: 10.1016/0370-2693(78)90429-X
1978HA48 Helv.Phys.Acta 51, 506 (1978) R.F.Haglund, Jr., R.E.Brown, N.Jarmie, G.G.Ohlsen, P.A.Schmelzbach, D.Fick Elastic Triton-Proton Scattering and Spin Dependent Nucleon-Nucleon Forces NUCLEAR REACTIONS 1H(polarized t, t), E(cm)=1.26, 1.68, 2.19, 2.70, 3.21, 3.71 MeV; measured σ(θ), A(θ); deduced phase shifts. Cluster model calculations.
1977BR21 Phys.Rev. C16, 513 (1977) R.E.Brown, G.G.Ohlsen, R.F.Haglund, Jr., N.Jarmie 3H(α, 6Li)n Reaction at 0° NUCLEAR REACTIONS 3He(α, α), (α, 6Li), (α, t), E=11.3-12.0 MeV; measured σ(E).
doi: 10.1103/PhysRevC.16.513
1977DO01 Phys.Rev. C15, 518 (1977) D.C.Dodder, G.M.Hale, N.Jarmie, J.H.Jett, P.W.Keaton, Jr., R.A.Nisley, K.Witte Elastic Scattering of Protons by Helium 4: New Experiments and Analysis NUCLEAR REACTIONS 4He(p, p), E=11-14 MeV; measured σ(E, θ); deduced R-matrix parameters for E=1-17 MeV.
doi: 10.1103/PhysRevC.15.518
1977HA17 Phys.Rev. C15, 1613 (1977) R.F.Haglund, Jr., G.G.Ohlsen, R.A.Hardekopf, N.Jarmie, R.E.Brown, P.A.Schmelzbach 3He(t, t)3He Elastic Scattering Measurements from 9 to 17 MeV NUCLEAR REACTIONS 3He(polarized t, t), E=9-17 MeV; measured σ(E, θ), A(E, θ).
doi: 10.1103/PhysRevC.15.1613
1977HA42 Phys.Rev. C16, 2151 (1977) R.F.Haglund, Jr., G.G.Ohlsen, R.A.Hardekopf, N.Jarmie, R.E.Brown Analyzing-Power Measurements for the 3He(t, d)4He Reaction NUCLEAR REACTIONS 3He(polarized t, d), E=9.02-17.27 MeV; measured A(E, θ).
doi: 10.1103/PhysRevC.16.2151
1977JA07 Phys.Rev. C16, 15 (1977) Neutron Source Reaction Cross Sections NUCLEAR REACTIONS 2H(d, 3He), E=12.305 MeV; measured σ(θ), θ(cm)=24-96°. 3H(p, 3He), E=13.600 MeV; measured σ(θ), θ(cm)=25-103°. 2H(t, α), E=20.000 MeV; measured σ(θ), θ=36-104°. θ=+-0.03°, Δσ=1%. Application to A=4, 5 systems.
doi: 10.1103/PhysRevC.16.15
1977JA12 Phys.Rev. C16, 2090 (1977) Statistical Analysis of 4He(p, p)4He Data NUCLEAR REACTIONS 4He(p, p), E ≤ 18 MeV; analyzed data. Statistical analysis of R-matrix analysis.
doi: 10.1103/PhysRevC.16.2090
1977TH05 Nucl.Phys. A283, 475 (1977) M.J.Throop, Y.T.Cheng, A.Goswami, O.Nalcioglu, D.K.McDaniels, L.W.Swenson, N.Jarmie, J.H.Jett, P.A.Lovoi, D.Stupin, G.G.Ohlsen, G.C.Salzman A Surface-Delta Description of Analyzing Power Measurements for Collective States of Ni and Zn Isotopes NUCLEAR REACTIONS 58,60Ni, 64Zn(polarized p, p'), E=15 MeV; measured σ(θ), A(θ). Enriched target, 98.0%.
doi: 10.1016/0375-9474(77)90553-X
1976HA17 Phys.Rev. C13, 2127 (1976) R.A.Hardekopf, G.G.Ohlsen, R.V.Poore, N.Jarmie Location of a Polarization Extremum in Triton-Alpha Scattering and its Application to a New Polarized Triton Source NUCLEAR REACTIONS 4He(polarized t, t), E=10.2-11.7 MeV; measured A(θ); deduced polarization extremum.
doi: 10.1103/PhysRevC.13.2127
1976JA09 Phys.Rev. C13, 2554 (1976) Proton-Proton Elastic Scattering at 19.700 MeV NUCLEAR REACTIONS 1H(p, p), E=19.7 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.13.2554
1976OH02 Phys.Rev. C14, 1688 (1976) G.G.Ohlsen, R.A.Hardekopf, N.Jarmie, R.V.Poore, R.L.Walter, P.W.Lisowski Polarized Triton Experiments on the Five-Nucleon System NUCLEAR REACTIONS 2H(polarized t, n), E=10.5 MeV; measured A(θ), polarization P(θ), polarization transfer coefficient. 2H(polarized t, n), E=5.4-15.7 MeV; measured polarization transfer coefficient. 2H(polarized t, t), E=10.5 MeV; measured A(θ).
doi: 10.1103/PhysRevC.14.1688
1976WI13 Phys.Rev. C14, 1545 (1976) H.B.Willard, B.D.Anderson, H.W.Baer, R.J.Barrett, P.R.Bevington, A.N.Anderson, H.Willmes, N.Jarmie Absolute Differential Cross Section Measurements for Proton-Proton Elastic Scattering at 647 and 800 MeV NUCLEAR REACTIONS 1H(p, p), E=647, 800 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.14.1545
1975BA35 Phys.Rev. C12, 451 (1975) B.P.Bayhurst, J.S.Gilmore, R.J.Prestwood, J.B.Wilhelmy, N.Jarmie, B.H.Erkkila, R.A.Hardekopf Cross Sections for (n, xn) Reactions between 7.5 and 28 MeV RADIOACTIVITY 189,190,193mIr; measured T1/2. NUCLEAR REACTIONS 27Al(n, α), E=21.4-26 MeV; measured σ(E, Eα). 45Sc, 89Y, 58Ni, 107Ag(n, 2n), 89Y, 107Ag, 151Eu, 191Ir(n, 3n), 151Eu, 191Ir(n, 4n), Zr(n, xn), E=14-28 MeV; 169Tm, 203Tl, 191,193Ir, 197Au(n, 2n), Lu(n, xn), 169Tm, 197Au, 203Tl(n, 3n), (n, 4n), E=8.6-28 MeV;193Ir(n, n), E=7.6-14.7 MeV;205Tl(n, 4n), E=23-28 MeV; measured σ(E). 90Zr, 175Lu(n, 2n), (n, 3n), 175Lu(n, 4n); calculated σ(E).
doi: 10.1103/PhysRevC.12.451
1975TH05 Phys.Rev.Lett. 35, 16 (1975) M.J.Throop, Y.T.Cheng, D.K.McDaniels, D.M.Stupin, L.W.Swenson, N.Jarmie, J.H.Jett, P.A.Lovoi, G.G.Ohlsen, G.C.Salzman Inelastic Proton Scattering as a Test of Surface-Delta Wave Functions NUCLEAR REACTIONS 58,60Ni, 64Zn(polarized p, p'), E=15 MeV; measured σ(Ep', θ), A(θ).
doi: 10.1103/PhysRevLett.35.16
1974DO05 Phys.Rev. C10, 571 (1974) T.R.Donoghue, G.G.Ohlsen, N.Jarmie, P.W.Keaton, Jr. Vector and Tensor Analyzing-Power Measurements for 3H(d, d)3H Elastic Scattering NUCLEAR REACTIONS 3H(polarized d, d), E=11.4, 14.4 MeV; measured A(θ).
doi: 10.1103/PhysRevC.10.571
1974JA15 Phys.Rev. C10, 54 (1974) Various Cross Sections for A ≤ 3 Nuclei NUCLEAR REACTIONS 1,3H(p, p), 3H(p, d), E=13.6 MeV; 2H(d, d), (d, p), E=12.3 MeV; 3He(d, d), (d, p), E=10 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.10.54
1974JA16 Phys.Rev. C10, 57 (1974) Polarized Protons on 3He at 13.6 MeV NUCLEAR REACTIONS 3He(polarized p, p), E=13.6 MeV; measured A(θ).
doi: 10.1103/PhysRevC.10.57
1974JA25 Phys.Rev. C10, 1748 (1974) N.Jarmie, J.H.Jett, R.J.Semper Elastic Scattering of Light Particles by Carbon, Oxygen, and Nitrogen NUCLEAR REACTIONS 12C, 14N, 16O(p, p), (d, d), (t, t), E=10-20 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.10.1748
1971DE19 Phys.Rev. C4, 52 (1971) J.L.Detch, Jr., R.L.Hutson, N.Jarmie, J.H.Jett Accurate Measurements of the Nuclear Processes T(p, p)T, T(p, 3He)n, T(p, d)D, and T(Polarized p, p)T from 13 to 20 MeV NUCLEAR REACTIONS 3H(p, p), (p, 3He), (p, d), (polarized p, p), E=13-20 MeV; measured σ(E;θ), P(θ); deduced phase shifts.
doi: 10.1103/PhysRevC.4.52
1971HU07 Phys.Rev. C4, 17 (1971) R.L.Hutson, N.Jarmie, J.L.Detch, Jr., J.H.Jett p-3He Elastic Scattering from 13 to 20 MeV NUCLEAR REACTIONS 3He(p, p), E=13-20 MeV; measured σ(E;θ); deduced phase shifts.
doi: 10.1103/PhysRevC.4.17
1971JA03 Phys.Rev. C3, 10 (1971) N.Jarmie, J.H.Jett, J.L.Detch, Jr., R.L.Hutson Proton-Proton Elastic Scattering from 9.6 to 13.6 MeV NUCLEAR REACTIONS 1H(p, p), E=9.6-13.6 MeV; measured σ(E;θ); deduced phase shifts.
doi: 10.1103/PhysRevC.3.10
1971JE01 Phys.Rev. C3, 1769 (1971) J.H.Jett, J.L.Detch, Jr., N.Jarmie d-4He Elastic Scattering at 12.000 MeV NUCLEAR REACTIONS 4He(d, d), E=12 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.3.1769
1970JA27 Phys.Rev.Lett. 25, 34 (1970) N.Jarmie, J.H.Jett, J.L.Detch, R.L.Hutson Proton-proton scattering at 9.690, 9.918 and 13.600 MeV NUCLEAR REACTIONS 1H(p, p), E=9.6-13.6 MeV; measured products, Ep, Ip; deduced σ(θ). Data were imported from EXFOR entry A1047.
doi: 10.1103/PhysRevLett.25.34
1967JA07 Phys.Rev. 161, 1050(1967) N.Jarmie, R.H.Stokes, G.G.Ohlsen, R.W.Newsome, Jr. Experimental Study of Excited 4H, 4He, and 4Li Nuclear Systems NUCLEAR STRUCTURE 4H, 3H, 3He, 4He, 4Li, 2H; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.161.1050
1963BU04 Bull.Am.Phys.Soc. 8, No.4, 317, G7 (1963) M.E.Bunker, M.G.Silbert, J.W.Starner, R.K.Sheline, N.Jarmie Decay of F21 NUCLEAR STRUCTURE 21F; measured not abstracted; deduced nuclear properties.
1963JA08 Phys.Rev. 130, 1987 (1963) N.Jarmie, M.G.Silbert, D.B.Smith, J.S.Loos Proton-Triton Elastic Scattering below 1 MeV NUCLEAR STRUCTURE 1H; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.130.1987
1963SM03 Phys.Rev. 129, 785 (1963) D.B.Smith, N.Jarmie, A.M.Lockett He3 + t Reactions NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.785
1961JA03 Bull.Am.Phys.Soc. 6, No.3, 237, DA12 (1961) N.Jarmie, M.G.Silbert, D.B.Smith N14(tn)O16*(p)N15, a Two-Stage Nuclear Reaction NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.
1961JA07 Phys.Rev. 123, 909 (1961) Nuclides Ar42 and Cl39 NUCLEAR STRUCTURE 39Cl, 42Ar; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.123.909
1961JA14 Nuclear Phys. 25, 443 (1961) N.Jarmie, M.G.Silbert, D.B.Smith The Two-Stage Nuclear Reaction N14(t, n)O16*(p)N15 NUCLEAR STRUCTURE 14N, 15N, 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90175-4
1961SI03 Phys.Rev. 123, 221 (1961) Nuclear Energy Levels of F19, F21, Ne22, and Ne24 NUCLEAR STRUCTURE 19F, 22Ne, 21F, 24Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.123.221
1961SI04 Nuclear Phys. 25, 438 (1961) M.G.Silbert, N.Jarmie, D.B.Smith Nuclear Energy Levels of N16 NUCLEAR STRUCTURE 16N, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90174-2
1960JA13 Phys.Rev. 120, 914 (1960) Nuclear Energy Levels of N17, O18, and O20 NUCLEAR STRUCTURE 17N, 20O, 18O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.120.914
1960JA19 Proc.Intern.Conf.Nuclear Structure, Kingston, Canada, D.A.Bromley, E.W.Vogt, Eds., University of Toronto Press, p.491 (1960) Energy Levels of N17, O18, and O20 NUCLEAR STRUCTURE 18O, 16O; measured not abstracted; deduced nuclear properties.
1959AJ77 Bull.Am.Phys.Soc. 4, No.4, 258, NA9 (1959) F.Ajzenberg-Selove, N.Jarmie, E.Haddad Neutrons from the Triton Bombardment of Li6 and Li7
1959JA01 Phys.Rev.Letters 3, 50 (1959) Oxygen-20
doi: 10.1103/PhysRevLett.3.50
1959JA16 Phys.Rev. 114, 176 (1959) T(p, p)T scattering near the T(p, n)3He threshold NUCLEAR REACTIONS 3H(p, p), E=703.5 keV-1.4 MeV; measured products, 3H; deduced σ(θ). Data were imported from EXFOR entry A1209.
doi: 10.1103/PhysRev.114.176
1958AL05 Phys.Rev. 111, 1129 (1958) Triton Reaction Cross Sections
doi: 10.1103/PhysRev.111.1129
1958JA05 Bull.Am.Phys.Soc. 3, No.8, 419, N11 (1958) T(p, p)T Scattering Near the T(p, n)He3 Threshold
1958JA06 Phys.Rev. 111, 1121 (1958) T(t, α)n, n Reaction
doi: 10.1103/PhysRev.111.1121
1957AL38 Bull.Am.Phys.Soc. 2, No.6, 305, E13 (1957) R.C.Allen, N.Jarmie, K.E.Brown T(t, α)n, n Reaction
1957JA37 LA-2014 (1957) Charged Particle Cross Sections Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1458. 1956JA31 Phys.Rev. 104, 1683 (1956) Energy Levels of O18 and F21
doi: 10.1103/PhysRev.104.1683
1955JA31 Phys.Rev. 98, 41 (1955) Excitation Function of O16(t, n)F18 NUCLEAR REACTIONS 16O(t, n), E=0.680-2.130 MeV; measured reaction products, Eβ, Iβ; deduced σ. Comparison with available data. RADIOACTIVITY 18F(β+); measured decay products, Eβ, Iβ; deduced T1/2. Comparison with available data.
doi: 10.1103/physrev.98.41
1955JA32 Phys.Rev. 99, 1043 (1955) Mass Measurement and Excited States of F21 NUCLEAR REACTIONS 19F(t, p), E=1.8 MeV; measured reaction products; deduced excited states, atomic mass. 2.5-MeV Van de Graaf accelerators and analazing the reaction products with a Cal-Tech type 16-inch double-focusing magnetic spectrometer.
doi: 10.1103/PhysRev.99.1043
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