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Search: Author = G.U.Din

Found 49 matches.

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1992DI02      Phys.Rev. C45, 2147 (1992)

G.U.Din, J.A.Cameron

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1989DI08      Phys.Rev. C40, 577 (1989)

G.U.Din, J.A.Cameron

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
Citations: PlumX Metrics


1988CA05      Phys.Rev. C37, 863 (1988)

J.A.Cameron, G.U.Din

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
Citations: PlumX Metrics


1988DI03      Phys.Rev. C38, 633 (1988)

G.U.Din, J.A.Cameron

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
Citations: PlumX Metrics


1988DI04      Phys.Rev. C38, 1164 (1988)

G.U.Din, J.A.Cameron

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
Citations: PlumX Metrics


1987DI01      Phys.Rev. C35, 448 (1987)

G.U.Din, J.A.Cameron

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1980HA36      Phys.Scr. 22, 439 (1980)

R.Hanninen, G.U.Din

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)

A.Osman, G.U.Din

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0208.


1979OS11      Ann.Phys.(Leipzig) 36, 64 (1979)

A.Osman, G.U.Din

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1080.


1978DI13      Aust.J.Phys. 31, 267 (1978)

G.U.Din

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
Citations: PlumX Metrics


1977DA18      Aust.J.Phys. 30, 167(1977)

J.R.Davis, G.U.Din

The 11B(3He, n0)13N Reaction

NUCLEAR REACTIONS 11B(3He, n), E=5-12 MeV; measured σ(E;En, θ).

doi: 10.1071/PH770167
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0206.


1977DI17      Aust.J.Phys. 30, 417 (1977)

G.U.Din, B.Heusch

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
Citations: PlumX Metrics


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)

G.U.Din, A.M.Al-Naser

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
Citations: PlumX Metrics


1975DI16      Aust.J.Phys. 28, 503 (1975)

G.U.Din, A.M.Al-Naser

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
Citations: PlumX Metrics


1975DI17      Aust.J.Phys. 28, 503 (1975)

G.U.Din, A.M.Al-Naser

A Study of Resonances in the 58Ni(p, γ)59Cu Reaction below 2.15 MeV

doi: 10.1071/PH750503
Citations: PlumX Metrics


1972DA02      Nucl.Phys. A179, 101 (1972)

J.R.Davis, G.U.Din

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0803.


1971DI12      Aust.J.Phys. 24, 139 (1971)

G.U.Din, J.L.Weil

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)

G.U.Din, J.R.Davis

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)

G.U.Din

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
Citations: PlumX Metrics


1969CO02      Nucl.Phys. A127, 95 (1969)

H.Cords, G.U.Din, B.A.Robson

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1065.


1969CO12      Nucl.Phys. A134, 561 (1969)

H.Cords, G.U.Din, B.A.Robson

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
Citations: PlumX Metrics


1969DI07      Nucl.Phys. A134, 655 (1969)

G.U.Din

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
Citations: PlumX Metrics


1969LE23      Australian J.Phys. 22, 669 (1969)

H.W.Lefevre, G.U.Din

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1479.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0223.


1967IV01      Nucl.Phys. A97, 177(1967)

M.Ivanovich, H.Cords, G.U.Din

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1966DI04      Nucl.Phys. 86, 509(1966)

G.U.Din, J.L.Weil

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0030.


1965DI07      Nucl.Phys. 73, 161 (1965)

G.U.Din, J.L.Weil

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
Citations: PlumX Metrics


1964DI02      Nucl.Phys. 50, 267 (1964)

G.U.Din, H.M.Kuan, T.W.Bonner

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1132.


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
Citations: PlumX Metrics


1963DI01      Bull.Am.Phys.Soc. 8, No.2, 115, I4 (1963)

G.U.Din, J.L.Weil

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)

H.Kuan, P.R.Almond, G.U.Din

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)

J.L.Weil, G.U.Din

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)

G.U.Din, H.M.Kuan, T.W.Bonner

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)

G.U.Din, H.Kuan, T.W.Bonner

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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Note: The following list of authors and aliases matches the search parameter G.U.Din: , G.U.DIN