NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = H.Rose Found 43 matches. 2023RO11 Phys.Rev. C 108, 025811 (2023) H.Rose, N.Kunert, T.Dietrich, P.T.H.Pang, R.Smith, C.Van Den Broeck, S.Gandolfi, I.Tews Revealing the strength of three-nucleon interactions with the proposed Einstein Telescope
doi: 10.1103/PhysRevC.108.025811
1986GA05 Rev.Roum.Phys. 31, 149 (1986) I.Garlea, Chr.Miron-Garlea, H.N.Rose, V.Raducu Measurement of Integral Cross Sections of (n, p) and (n, α) Reactions for 98Mo, 64Zn, 59Co, 54Fe and 93Nb Isotopes, at 14.8 MeV NUCLEAR REACTIONS 98Mo, 64Zn, 59Co, 54Fe, 93Nb(n, p), (n, α), E=14.8 MeV; measured reaction σ. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30807. 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
1960TA22 J.Nuclear Energy 12A, 16 (1960) R.B.Tattersall, H.Rose, S.K.Pattenden, D.Jowitt
1960TA29 J.Nucl.Energy: Pt.A, 12, 32 (1960) R.B.Tattersall, H.Rose, S.K.Pattenden, D.Jowitt Pile Oscillator Measurements of Resonance Absorption Integrals Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20638. 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
1959RO60 Progr.In Nuclear Energy 3, 292 (1959) H.Rose, W.A.Cooper, R.B.Tattersall
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
1953RO10 Phil.Mag. 44, 739 (1953) The Beta-Gamma Angular Correlation of 76Arsenic
doi: 10.1080/14786440708521051
1952RI01 Proc.Phys.Soc.(London) 65, 484 (1952) The Decay of 188Re RADIOACTIVITY 186Re(β-), (EC); 188Re(β-) [from Re neutron irradiation]; measured β spectra, I(ce), γγ-, βγ-coin. 188Os deduced transitions, γ-branching.
doi: 10.1088/0370-1298/65/7/304
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