NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = H.J.Rose Found 36 matches. 1984RO30 Nature(London) 307, 245 (1984) A New Kind of Natural Radioactivity RADIOACTIVITY 223Ra(α), (14C); measured relative branching ratios. Discussed other nuclei decay data.
doi: 10.1038/307245a0
1973CO38 Nucl.Phys. A217, 400 (1973) A.J.Cox, J.M.G.Caraca, B.Schlenk, R.D.Gill, H.J.Rose Electromagnetic Transitions in 42Ti NUCLEAR REACTIONS 40Ca(3He, nγ), E=8.0 MeV; measured Doppler-shift attenuation, (θ(n)=0°, θ(γ)), Eγ. 42Ti levels deduced T1/2, level-width, γ-multipolarities. Natural targets.
doi: 10.1016/0375-9474(73)90203-0
1972CA22 Nucl.Phys. A193, 1 (1972) J.M.G.Caraca, R.D.Gill, A.J.Cox, H.J.Rose Gamma Decay of Low-Lying States in 30S and 34Ar NUCLEAR REACTIONS 28Si(3He, n), 32S(3He, n), E=6.5-10 MeV; measured Doppler-shift attenuation, (θ(n)=0°, θ(γ)), Eγ. 30S, 34Ar deduced T1/2. Natural targets.
doi: 10.1016/0375-9474(72)90230-8
1972GI01 Nucl.Phys. A180, 79 (1972) R.D.Gill, J.M.G.Caraca, A.J.Cox, H.J.Rose Gamma-Decay Modes of 18Ne NUCLEAR REACTIONS 16O(3He, n), E=10.3-10.8 MeV;measured Doppler-shift recoil distance. 18Ne deduced T1/2, branching ratios, γ-mixing. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(72)90157-1
1972GI06 Nucl.Phys. A187, 369 (1972) R.D.Gill, J.M.G.Caraca, A.J.Cox, H.J.Rose Transition Rates in 89Zr NUCLEAR REACTIONS 89Y(p, nγ)89Zr, Ep=5.26-6.42 MeV; measured σ(E;Eγ, θ(γ)), Doppler-shift attenuation. 89Zr deduced levels, T1/2, branching ratios. Natural targets; Ge(Li) detector.
doi: 10.1016/0375-9474(72)90583-0
1971CA40 Nucl.Phys. A176, 273 (1971) J.M.G.Caraca, R.D.Gill, P.B.Johnson, H.J.Rose Transition Strengths in 37Ar and 35Cl NUCLEAR REACTIONS 37Cl(p, nγ), 35Cl(p, p'), E=4.15-6.15 MeV; measured Doppler-shift attenuation. 37Ar, 35Cl deduced T1/2. Natural target.
doi: 10.1016/0375-9474(71)90269-7
1971RO18 Particles and Nuclei 1, 453 (1971) H.J.Rose, R.D.Gill, J.M.G.Caraca, A.J.Cox The 'Open' Question of the 0+ State in 18Ne NUCLEAR REACTIONS 16O(3He, nγ), E=10.3 MeV; measured σ(En, Eγ). 18Ne deduced first excited 0+ state, cross-over transition.
1970GI09 Nucl.Phys. A152, 369 (1970) R.D.Gill, K.Bharuth-Ram, K.P.Jackson, R.A.I.Bell, B.C.Robertson, J.L'Ecuyer, N.G.Chapman, H.J.Rose Electromagnetic Transitions in 19Ne NUCLEAR REACTIONS 19F(p, n), E=8.48-10.4 MeV; 16O(α, n), E=15-19 MeV; measured σ(E;En, Eγ, θ(nγ)), Doppler shift attenuation. 19Ne deduced levels, T1/2, branching ratios, J, π, γ-mixing. Natural targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(70)90837-7
1969BE31 Nucl.Phys. A133, 337(1969) R.A.L.Bell, J.L'Ecuyer, R.D.Gill, B.C.Robertson, I.S.Towner, H.J.Rose Excitation Energies and Lifetimes of Levels in 26Si NUCLEAR REACTIONS 24Mg(3He, nγ); E = 5.5, 7.8, 10 MeV; measured σ(E; Eγ, θ(n), θ(p)), γγ-coin, Doppler shift attenuation. 26Si deduced levels, T1/2 branching ratios, J, π, transition strengths. Enriched (99.8%) target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90636-8
1969RO08 Nucl.Phys. A126, 431(1969) B.C.Robertson, R.A.I.Bell, J.L'Ecuyer, R.D.Gill, H.J.Rose A Study of the Gamma Rays in 18Ne NUCLEAR REACTIONS 16O(3He, n); E=8.5-13.15 MeV; measured σ(Eγ, θ(nγ)), Eγ, Doppler shift attenuation. 18Ne deduced levels, T1/2, γ-branching ratios, J, delta. Natural target; Ge(Li) detector.
doi: 10.1016/0375-9474(69)90477-1
1969RO15 Nucl.Phys. A132, 481 (1969) B.C.Robertson, R.D.Gill, R.A.I.Bell, J.L'Ecuyer, H.J.Rose Lifetimes of 39K Excited States: the 2s1/2 Hole State NUCLEAR REACTIONS 39K(p, p'), E=8.175 MeV; measured Eγ, Doppler shift attenuation. 39K levels deduced T1/2. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90713-1
1968BE30 Nucl.Phys. A118, 481(1968) R.A.I.Bell, R.D.Gill, B.C.Robertson, J.S.Lopes, H.J.Rose Electromagnetic Transitions in 11B and 14C NUCLEAR REACTIONS 12C(t, α), (t, p), E=7.48, 7.68 MeV; measured Iγ(Eα, Eγ, θ(αγ)), Iγ(Ep, Eγ, θ(pγ)). 11B, 14C levels; deduced J, γ-branching, delta. Natural target.
doi: 10.1016/0375-9474(68)90434-X
1968GI01 Nucl.Phys. A106, 678 (1968) R.D.Gill, J.S.Lopes, B.C.Robertson, R.A.I.Bell, H.J.Rose A Study of Positive-Parity States in 15O NUCLEAR REACTIONS 16O(3He, αγ), E = 9.1 MeV; measured σ(Eα, Eγ, θ(αγ)). 15O levels deduced J, delta. Natural target.
doi: 10.1016/0375-9474(68)90523-X
1968GI04 Nucl.Phys. A114, 416(1968) R.D.Gill, G.P.Littlewood, J.S.Lopes, H.J.Rose Electromagnetic Properties of Low-Lying Levels of 31Si NUCLEAR REACTIONS 30Si(d, pγ), E=2.95-4.00 MeV; measured σ(Ep, θ(p)=180°, θ(γ)). 31Si deduced levels J, delta. Enriched target.
doi: 10.1016/0375-9474(68)90364-3
1968GI09 Phys.Letters 28B, 116 (1968) R.D.Gill, B.C.Robertson, J.L'Ecuyer, R.A.I.Bell, H.J.Rose Lifetime Measurements in 18Ne NUCLEAR REACTIONS 16O(3He, nγ), E=12 MeV; measured nγ-coin, Doppler shift attenuation. 18Ne deduced levels, J, π, T1/2.
doi: 10.1016/0370-2693(68)90146-9
1968GI11 Nucl.Phys. A121, 209 (1968) R.D.Gill, J.S.Lopes, O.Hausser, H.J.Rose Lifetime Measurements in Mass-15 Nuclei NUCLEAR REACTIONS 2H(14N, 15O), 2H(14N, 15N), E=21.8 MeV; measured Eγ, Doppler shift attenuation. 15N, 15O levels deduced T1/2. Enriched targets, Ge(Li) detector.
doi: 10.1016/0375-9474(68)90509-5
1968LO03 Nucl.Phys. A109, 241(1968) J.S.Lopes, B.C.Robertson, R.D.Gill, R.A.I.Bell, H.J.Rose Electromagnetic Properties of 39K Bound States NUCLEAR REACTIONS 42Ca(p, αγ), E=10.6-11.1 MeV; 39K(p, p'γ), E=7.12-8.51 MeV; measured σ(E; Eγ, θ(γ)). 39K, deduced J, multipole mixing ratios. Enriched targets.
doi: 10.1016/0375-9474(68)90592-7
1967GI07 Nucl.Phys. A98, 129(1967) R.D.Gill, O.Hausser, J.S.Lopes, H.J.Rose The Decay of the 8.88 MeV Level in 16O NUCLEAR REACTIONS 19F(p, αγ), E = 7.4 MeV; measured σ(Eα, Eγ, θ(αγ)). 16O deduced levels, branching, transition mixing ratios.
doi: 10.1016/0375-9474(67)90904-9
1967RO21 Rev.Mod.Phys. 39, 306 (1967) Angular Distributions of Gamma Rays in Terms of Phase-Defined Reduced Matrix Elements
doi: 10.1103/RevModPhys.39.306
1966HA30 Nucl.Phys. 84, 683(1966) O.Hausser, R.D.Gill, J.S.Lopes, H.J.Rose Gamma Rays from Positive Parity States in 15N NUCLEAR REACTIONS 18O(p, αγ), E = 8.50-9.25 MeV; measured σ(Eα, θ(α) = 180°, θ(γ)). 15N deduced J, mixing ratios. Enriched target.
doi: 10.1016/0029-5582(66)91025-X
1966HA31 Phys.Letters 22, 604 (1966) O.Hausser, H.J.Rose, J.S.Lopes, R.D.Gill Comparison of Signs of Mixing Ratios to Model Predictions NUCLEAR STRUCTURE 15N, 16O, 14N, 18F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90674-3
1966LO02 Nucl.Phys. 76, 223 (1966) J.S.Lopes, O.Hausser, H.J.Rose, A.R.Poletti, M.F.Thomas The 3/2 → 1/2 Hole Transitions in Mass 15 NUCLEAR REACTIONS 16O(3He, αγ), E = 8.1 MeV, natural target; 18O(p, αγ), E = 8.6 MeV, enriched target; measured σ(Eα, θ(α) = 180°, θ(γ)). 15O, 15N deduced J, γ-mixing.
doi: 10.1016/0029-5582(66)90970-9
1966LO12 Nucl.Phys. 89, 127(1966) J.S.Lopes, O.Hausser, R.D.Gill, H.J.Rose Properties of Bound States of 18O Above the 4.45 MeV State NUCLEAR REACTIONS 18O(p, p'γ), E = 7.9-10.0 MeV; measured σ(Ep, θ(p) = 180°, θ(γ)), Eγ, Iγ. 18O deduced J, π, multipolarity mixing ratios. Enriched target.
doi: 10.1016/0029-5582(66)90849-2
1965RI02 Phys.Rev. 137, B507 (1965) F.Riess, W.Trost, H.J.Rose, E.K.Warburton Quadrupole-Dipole Mixture of the N14 3.95→0 gamma-Ray Transition NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.137.B507
1964RO03 Nucl.Phys. 52, 481 (1964) The 10.43 MeV State in N14 NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90709-6
1964TR04 Phys.Letters 10, 83 (1964) Direct Radiative Capture of Protons into the Lowest Odd-Parity States of N14 NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90588-8
1963RO17 Nucl.Phys. 44, 287 (1963) The Gamma Decay of the 10.22 MeV State in N14 NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90027-0
1962RO21 Nuclear Phys. 36, 583 (1962) H.J.Rose, F.Uihlein, F.Riess, W.Trost Polarization Measurements on the 5.83 → 5.10 MeV Gamma Transition in N14 NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90485-6
1960RO13 Nuclear Phys. 19, 113 (1960) The Decay of Modes of the 9.17-MeV Excited State in N14 NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90225-X
1960RO23 Nuclear Phys. 21, 367 (1960) Ground State Gamma Transtions from States at 10.09 and 10.24 MeV in N14 and Reinvestigation of the 9.17- and 10.43-MeV Gamma Ray Distributions NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90062-6
1959RO54 Nuclear Phys. 12, 510 (1959) The Spin Assignments of the 9.16 MeV and 6.44-MeV States in N14
doi: 10.1016/0029-5582(59)90024-0
1959RO63 Thesis, Freiburg Br., Albert-Ludwigs-Univ. (1959); Nuclear Sci.Abstr. 17, 319, Abstr. 2329 (1963)
1959WA01 Phys.Rev.Letters 2, 238 (1959) E.K.Warburton, H.J.Rose, E.N.Hatch C13(p, γ)N14 1.47- and 2.11-MeV Resonances and the Odd-Parity Levels of Mass 14
doi: 10.1103/PhysRevLett.2.238
1959WA02 Bull.Am.Phys.Soc. 4, No.4, 219, AB9 (1959) E.K.Warburton, W.T.Pinkston, H.J.Rose, E.N.Hatch Direct Radiative Capture of Protons by C13
1959WA04 Phys.Rev. 114, 214 (1959) E.K.Warburton, H.J.Rose, E.N.Hatch C12(p, γ)N14 1.47- and 2.11-MeV Resonances and the Odd-Parity Levels of Mass 14
doi: 10.1103/PhysRev.114.214
1958WA02 Phys.Rev. 109, 1199 (1958) Gamma Rays from C13 + d and the Excited States of C14
doi: 10.1103/PhysRev.109.1199
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