NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = G.U.Din Found 49 matches. 1992DI02 Phys.Rev. C45, 2147 (1992) Reaction 48Ti(p, γ)49V from 1.75 to 2.50 MeV NUCLEAR REACTIONS 48Ti(p, γ), E=1.75-2.5 MeV; measured Eγ, Iγ. 49V deduced resonances, J, π, γ-decay branching.
doi: 10.1103/PhysRevC.45.2147
1991DI07 Phys.Rev. C44, 972 (1991) G.U.Din, I.A.Al-Agil, A.M.A.Al-Soraya, J.A.Cameron Reaction 52Cr(p, γ)53Mn from 1.66 to 2.91 MeV NUCLEAR REACTIONS, ICPND 52Cr(p, γ), E=1.66-2.91 MeV; measured γ-yield, Iγ(θ). 53Mn deduced resonances, J, π, IAS.
doi: 10.1103/PhysRevC.44.972
1990AL22 Phys.Rev. C42, 530 (1990) I.A.Al-Agil, G.U.Din, A.M.A.Al-Soraya, S.A.Bagazi, J.A.Cameron Reaction 52Cr(p, γ)53Mn from 1.38 to 1.66 MeV NUCLEAR REACTIONS, ICPND 52Cr(p, γ), E=1.38-1.66 MeV; measured γ yield, Eγ, Iγ, γ(θ). 53Mn deduced levels, J, π, γ-branching, analog state Γγ, C2S.
doi: 10.1103/PhysRevC.42.530
1990HA43 Can.J.Phys. 68, 1322 (1990) E.E.Habib, J.A.Cameron, G.U.Din, V.Janzen, R.Schubank Low-Lying States in 97Mo and 101Mo by (t, d) and (d, p) Reactions on the Neighbouring Molybdenum Isotopes NUCLEAR REACTIONS 96,100Mo(polarized d, p), E=12 MeV; 96,100Mo(t, d), E=14 MeV; measured σ(θ), σ(Ep), σ(Et), vector analyzing power. 97,101Mo deduced levels, J, π, spectroscopic factors.
doi: 10.1139/p90-189
1989DI08 Phys.Rev. C40, 577 (1989) Reactions 54Fe(p, γ)55Co and 54Fe(p, p'γ)54Fe from 2.35 to 3.90 MeV NUCLEAR REACTIONS 54Fe(p, γ), (p, p'γ), E=2.1-3.9 MeV; measured Eγ, Iγ, γ yield, γ(θ). 55Co deduced levels, J, π, IAS.
doi: 10.1103/PhysRevC.40.577
1988CA05 Phys.Rev. C37, 863 (1988) Low-Lying l = 3 Proton Resonances in 50Cr + p NUCLEAR REACTIONS 50Cr(p, γ), E=1-1.5 MeV; measured Eγ, Iγ, γ(θ). 51Mn deduced resonances, J, π, analogs.
doi: 10.1103/PhysRevC.37.863
1988DI03 Phys.Rev. C38, 633 (1988) Reactions 50Cr(p, γ)51Mn and 50Cr(p, p'γ)50Cr from 2.5 to 3.1 MeV NUCLEAR REACTIONS 50Cr(p, γ), (p, p'γ), E=2.5-3.1 MeV; measured Iγ(Ep), Iγ(θ), γ yield. 51Mn deduced proton resonances J, π, analogs.
doi: 10.1103/PhysRevC.38.633
1988DI04 Phys.Rev. C38, 1164 (1988) g9/2 Isobaric Analog State in 55Co NUCLEAR REACTIONS 54Fe(p, p'γ), E ≈ 3.45-3.475 MeV; measured yield curves, γ(θ). 55Co deduced levels, J, π, g9/2 IAR fragmentation.
doi: 10.1103/PhysRevC.38.1164
1987DI01 Phys.Rev. C35, 448 (1987) d5/2 Isobaric Analog State in 55Co NUCLEAR REACTIONS 54Fe(p, p'γ), E=3.88-4.28 MeV; measured σ(E), γ(θ), Eγ, Iγ, γ yield vs E. 55Co deduced resonances, J, π, Γp, Γγ, IAR fragmentation, γ-branching. Enriched target, Ge detector.
doi: 10.1103/PhysRevC.35.448
1986DI01 Phys.Rev. C33, 103 (1986) G.U.Din, A.M.Al Soraya, J.A.Cameron, V.P.Janzen, R.B.Schubank Reactions 50Cr(p, γ)51Mn and 50Cr(p, p'γ)50Cr from 1.7 to 2.5 MeV NUCLEAR REACTIONS, ICPND 50Cr(p, γ), (p, p'γ), E=1.7-2.5 MeV; measured Iγ(Ep), Eγ, γ(θ), γ yields. 51Mn deduced levels, J, π, γ-branching ratios, δ, IAR. Ge detector.
doi: 10.1103/PhysRevC.33.103
1985DI05 Phys.Rev. C31, 800 (1985) G.U.Din, J.A.Cameron, V.P.Janzen, R.B.Schubank Reactions 58Ni(p, γ)59Cu and 58Ni(p, p'γ)58Ni from 0.75 to 5.00 MeV NUCLEAR REACTIONS, ICPND 58Ni(p, γ), (p, p'γ), E=0.75-5 MeV; measured yield vs E, Eγ, γ(θ). 59Cu deduced levels, J, π, IAR.
doi: 10.1103/PhysRevC.31.800
1985DI09 Phys.Rev. C31, 1566 (1985) G.U.Din, A.M.AlSoraya, J.A.Cameron, J.Sziklai Low-Lying Proton Resonances of Spin (9/2) in 51Mn and 53Mn NUCLEAR REACTIONS 50Cr(p, γ), E=2.39 MeV; 52Cr(p, γ), E=2.68 MeV; measured Iγ(E, Eγ), Iγ(θ), γ yield. 51,53Mn deduced resonances, J, π.
doi: 10.1103/PhysRevC.31.1566
1982DI11 Nucl.Phys. A385, 256 (1982) G.U.Din, J.A.Cameron, V.Janzen, R.Schubank Analogue Resonances in 19F NUCLEAR REACTIONS 18O(p, p'γ), (p, nγ), (p, αγ), E=4.4-4.62, 4.75-4.83, 5-5.66 MeV; measured yields, σ(E), γ(θ). 19F deduced resonances, J, π, IAS.
doi: 10.1016/0375-9474(82)90171-3
1982HA41 Phys.Rev. C26, 834 (1982) E.E.Habib, J.A.Cameron, G.U.Din, V.Janzen, R.Schubank Determination of the Spins and Parities of Low-Lying States in 99Mo by Means of the 100Mo(d(pol), t)99Mo and 98Mo(d(pol), p)99Mo Reactions NUCLEAR REACTIONS 100Mo(polarized d, t), 98Mo(polarized d, p), E=16 MeV; measured σ(θ), σ(Ep), σ(Et); deduced optical model parameters. 99Mo levels deduced J, π, S.
doi: 10.1103/PhysRevC.26.834
1980HA36 Phys.Scr. 22, 439 (1980) Investigation of 55Co Levels with the 54Fe(p, γ)55Co Reaction I. Excitation and Decay Properties of Resonances NUCLEAR REACTIONS 54Fe(p, γ), E=0.8-2.37 MeV; measured Eγ, Iγ; deduced Q. 55Co deduced resonances, resonance strength, γ-branching ratio, E1, E2, M1, M2 transition probabilities.
1980HA37 Phys.Scr. 22, 451 (1980) R.Hanninen, R.Hentela, G.U.Din Investigation of 55Co Levels with the 54Fe(p, γ)55Co Reaction II. Spins and Lifetimes NUCLEAR REACTIONS 54Fe(p, γ), E=1.1-2.3 MeV; measured Iγ(θ), DSA. 55Co levels deduced J, π, T1/2, δ.
1979OS10 Ann.Phys.(Leipzig) 36, 56 (1979) 9Be(3He, n)11C and 11B(3He, n)13N Reactions at Energies below Coulomb Barrier NUCLEAR REACTIONS 9Be, 11B(3He, n), E=0.9-1.9 MeV; measured σ(θ). Coulomb distorted wave calculations.
doi: 10.1002/andp.19794910110
1979OS11 Ann.Phys.(Leipzig) 36, 64 (1979) The (d, p) Reactions below 3.0 MeV NUCLEAR REACTIONS 12C, 23Na, 27Al(d, p), E=1.5-3 MeV; measured σ(E, θ). Subcoulomb barrier stripping theory.
doi: 10.1002/andp.19794910111
1978DI13 Aust.J.Phys. 31, 267 (1978) 16O(p, γ)19F and 18O(p, p'γ)18O Reactions below 3.50 MeV NUCLEAR REACTIONS 18O(p, γ), 18O(p, p'γ), E < 3.50 MeV; measured Eγ, Iγ, γ(θ). 19F deduced levels, resonances, J, π, T, branching ratio.
doi: 10.1071/PH780267
1977DA18 Aust.J.Phys. 30, 167(1977) The 11B(3He, n0)13N Reaction NUCLEAR REACTIONS 11B(3He, n), E=5-12 MeV; measured σ(E;En, θ).
doi: 10.1071/PH770167
1977DI17 Aust.J.Phys. 30, 417 (1977) A Study of the 42Ca(p, γ)43Sc Reaction NUCLEAR REACTIONS 42Ca(p, γ), E < 2.75 MeV; measured Eγ, Iγ, γ(θ). 43Sc deduced resonances, levels, J, π, γ-branching.
doi: 10.1071/PH770417
1976AW02 Nucl.Sci.Appl., Ser.B 9, 1 (1976) M.A.Awal, H.M.Sen Gupta, G.U.Din Energy Levels of 55Co from 54Fe(p, γ)55Co Reaction NUCLEAR REACTIONS 54Fe(p, γ), E=1286, 1680, 1747 keV; measured Eγ, Iγ. 55Co deduced levels, transitions.
1975DI10 Aust.J.Phys. 28, 263 (1975) 50Cr(p, γ)51Mn Reaction from E = 1.45 to 2.07 MeV NUCLEAR REACTIONS 50Cr(p, γ), E=1.45-2.07 MeV; measured σ(E, Eγ, θ); deduced Q. 51Mn deduced levels, J, π, δ, γ-branching.
doi: 10.1071/PH750263
1975DI16 Aust.J.Phys. 28, 503 (1975) A Study of Resonances in the 58Ni(p, γ)59Cu Reaction below 2.15 MeV NUCLEAR REACTIONS 58Ni(p, γ), E=1400-2150 keV; measured σ(E, Eγ); deduced Q. 59Cu deduced levels, resonances, γ-branching.
doi: 10.1071/PH750503
1975DI17 Aust.J.Phys. 28, 503 (1975) A Study of Resonances in the 58Ni(p, γ)59Cu Reaction below 2.15 MeV
doi: 10.1071/PH750503
1972DA02 Nucl.Phys. A179, 101 (1972) The 12C(d, n0)13N Reaction from 3.6 MeV to 12.0 MeV NUCLEAR REACTIONS 12C(d, n0), E=3.6-12 MeV; measured σ(E:θ), σ(En, θ). Natural target.
doi: 10.1016/0375-9474(72)90108-X
1971DI12 Aust.J.Phys. 24, 139 (1971) The 18O(3He, n0)20Ne and 18O(3He, n1)20Ne Reactions from 2.0 to 4.6 MeV NUCLEAR REACTIONS 18O(3He, n), E=2-4.6 MeV; measured σ(E;θ); deduced reaction mechanism.
1971DI21 Aust.J.Phys. 24, 497 (1971) A Study of Resonances in the 29Si(p, γ)30P Reaction NUCLEAR REACTIONS 29Si(p, γ), E=900-2120 keV; measured σ(E;Eγ). 30P deduced resonances, levels, J, π, T, γ-branching. Ge(Li) detectors.
1970DI07 Aust.J.Phys. 23, 261 (1970) The 29Si(p, γ)30P and 29Si(p, p'γ)29Si Reactions from 1300 to 1850 keV NUCLEAR REACTIONS 29Si(p, γ), (p, p'γ), E=1.30-1.85 MeV; measured σ(E;Eγ), Iγ. 30P deduced resonances, level-width, γ-branching.
1970KN03 Phys.Rev.Lett. 25, 1210 (1970) D.W.Kneff, H.W.Lefevre, G.U.Din Reaction Q Values from Near-Threshold Neutron Spectra NUCLEAR REACTIONS 41K, 45Sc, 51V, 57Fe(p, n), E near threshold; measured σ(E;En); deduced Q.
doi: 10.1103/PhysRevLett.25.1210
1969CO02 Nucl.Phys. A127, 95 (1969) Deuteron-Induced Reactions in 12C at Bombarding Energies of 5 to 10 MeV NUCLEAR REACTIONS 12C(d, d), (d, p), (d, α), E=5 to 10 MeV; measured σ(E, θ), σ(E;Ep, θ), σ(E;Eα, θ). Natural target.
doi: 10.1016/0375-9474(69)90770-2
1969CO12 Nucl.Phys. A134, 561 (1969) Tensor Polarization and Reactions of Deuterons on 16O at Bombarding Energies of 4.4 to 8.4 MeV NUCLEAR REACTIONS 16O(d, d), (d, p), (d, α), E = 4.4 to 8.4 MeV; measured tensor polarization (θ), σ(E, θ). Natural target.
doi: 10.1016/0375-9474(69)90022-0
1969DI07 Nucl.Phys. A134, 655 (1969) Proton-Induced Reactions in 18O from 3.00 to 7.00 MeV NUCLEAR REACTIONS 18O(p, p'γ), 18O(p, αγ), 18O(p, nγ), E = 3.0 to 7.0 MeV; measured σ(E, θ). 19F deduced levels. Isotopic target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90028-1
1969LE23 Australian J.Phys. 22, 669 (1969) Zero Degree Neutron Yield from the 7Li(p, n)7Be Reaction Near 2.2 MeV NUCLEAR REACTIONS 7Li(p, n), E=1.93-2.7 MeV; measured σ(E;En).
doi: 10.1071/PH690669
1968CO10 Nucl.Phys. A113, 608(1968) H.Cords, G.U.Din, M.Ivanovich, B.A.Robson Tensor Polarization of Deuterons from 12C-d Elastic Scattering NUCLEAR REACTIONS 12C(d, d), E=3.5 to 7.1 MeV; measured tensor polarization (E, θ). Natural target.
doi: 10.1016/0375-9474(68)90170-X
1967DI01 Nucl.Phys. A93, 190(1967) G.U.Din, M.A.Nagarajan, R.Pollard The Study of 10B(d, n)11C and 11B(d, n)12C Reactions NUCLEAR REACTIONS 10B(d, n), E = 3.2 to 9 MeV; measured σ(E; En, θ); 11B(d, n), E = 1.1 to 2.9 MeV; measured σ(E; En). Enriched targets.
doi: 10.1016/0375-9474(67)90179-0
1967IV01 Nucl.Phys. A97, 177(1967) Deuteron Tensor Polarization in the 9Be(p, d)8Be Reaction NUCLEAR REACTIONS 9Be(p, d), E = 4.9 to 9.8 MeV; measured tensor polarization (E, θ). Natural target.
doi: 10.1016/0375-9474(67)90777-4
1967PR04 Phys.Rev. 157, 779 (1967) F.W.Prosser, Jr., G.U.Din, D.D.Tolbert Study of the Reactions O18(p, n)F18, O18(p, p'γ)O18, and O18(p, αγ)N15 from E = 2500 to 3000 keV NUCLEAR STRUCTURE 18O, 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.157.779
1966DI04 Nucl.Phys. 86, 509(1966) The Reactions 11B(3He, N)13N and 7Li(3He, N)9B from 1.5 to 5.5 MeV Bombarding Energy NUCLEAR REACTIONS 7Li, 11B(3He, n0), E = 1.5-5.5 MeV; measured σ(E, θ). 10B, 14N deduced levels, level-width. Enriched targets.
doi: 10.1016/0029-5582(66)90493-7
1965DI07 Nucl.Phys. 73, 161 (1965) The 13C(3He, n0)15O Reaction at 1.4 to 5.8 MeV NUCLEAR REACTIONS 13C(3He, n), E = 1.4-5.8 MeV; measured σ(E;θ n). Enriched target.
doi: 10.1016/0029-5582(65)90163-X
1964DI02 Nucl.Phys. 50, 267 (1964) Excitation functions and angular distributions for the reaction C12(He3, n)O14 NUCLEAR REACTIONS 12C(3He, n), E=1.8-5.5 MeV; measured reaction products, Eγ, Iγ; deduced σ(θ).
doi: 10.1016/0029-5582(64)90206-8
1964KU09 Nucl.Phys. 60, 509(1964) H.-M.Kuan, P.R.Almond, G.U.Din, T.W.Bonner The 15.1 MeV Gamma-Ray Excitation Functions of the Reactions B10(He3, pγ15. 1)C12, B11(d, nγ15. 1)Cr12 and C13(He3, αγ15. 1)C12 NUCLEAR REACTIONS 10B(3He, pγ), E(3He)=1.8-5.5 MeV; 11B(d, nγ), Ed=1.5-5.5 MeV; 13C(3He, αγ), E(3He)=2-5 MeV; measured σ. 13N, 13C, 16O deduced resonance parameters.
doi: 10.1016/0029-5582(64)90027-6
1963DI01 Bull.Am.Phys.Soc. 8, No.2, 115, I4 (1963) Excitation Functions of Li7(He3, n)B9 and O18(He3, n)Ne20 and the Angular Distribution of O18(He3, n)Ne20 NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1962KU02 Bull.Am.Phys.Soc. 7, No.2, 111, A4 (1962) Excitation Curves of 15.1-MeV Gamma Rays from B10(He3, pγ)C12, and C13(He3, αγ)C12
1962WE01 Bull.Am.Phys.Soc. 7, No.1, 59, R5 (1962) J.L.Weil, G.U.Din, H.M.Kuan, P.R.Almond Be9(He3, n)C11 Reaction NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1962WE03 Bull.Am.Phys.Soc. 7, No.2, 111, A5 (1962) B11(He3, n)N13 and C13(He3, n)O15 Reactions NUCLEAR STRUCTURE 11B, 13C; measured not abstracted; deduced nuclear properties.
1961DI02 Bull.Am.Phys.Soc. 6, No.3, 236, DA5 (1961) Excitation Curves and Angular Distributions for the Reaction C12(He3, n)O14 NUCLEAR STRUCTURE 15O; measured not abstracted; deduced nuclear properties.
1961DI08 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.499 (1961) Mechanism of the Reaction C12(He3, n)O14 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1960RE02 Bull.Am.Phys.Soc. 5, No.2, 110, N3 (1960) T.Retz-Schmidt, T.W.Bonner, G.U.Din, J.L.Weil Absolute Yields of Neutron Groups from Be9(α, n)C12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
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