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NSR database version of May 3, 2024.

Search: Author = G.Kennedy

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2021LI05      J.Radioanal.Nucl.Chem. 327, 533 (2021)

X.Li, R.van Sluijs, G.Kennedy

Measurement of k_o values for europium, lutetium and iridium at FRM II with a very well thermalized neutron spectrum

NUCLEAR REACTIONS ^152,154Eu, ¹⁷⁷Lu, ^192,194Ir(n, γ), E thermal; measured reaction products; deduced Westcott factors. Comparison with available data.

doi: 10.1007/s10967-020-07500-2
Citations: PlumX Metrics

2014CH18      J.Radioanal.Nucl.Chem. 300, 609 (2014)

C.Chilian, L.Sneyers, P.Vermaercke, G.Kennedy

Measurement k₀ and Q₀ values for iridium isotopes

NUCLEAR REACTIONS ^191,193Ir(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced k₀ factor, Q₀. Comparison with available data.

doi: 10.1007/s10967-014-3023-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23235.

2014VA01      J.Radioanal.Nucl.Chem. 300, 539 (2014)

R.van Sluijs, R.Jacimovic, G.Kennedy

A simplified method to replace the Westcott formalism in k₀NAA using non-1/ν nuclides

NUCLEAR REACTIONS ¹⁷⁶Lu, ¹⁶⁸Yb, ¹⁰³Rh, ¹⁹³Ir, ¹¹⁵In, ¹⁹⁷Au, ^185,187Re, ¹⁶⁴Dy, ¹⁷⁵Lu, ^151,153Eu(n, γ), E not given; calculated Westcott factors, σ. Hogdahl convention, comparison with available data.

doi: 10.1007/s10967-014-2958-8
Citations: PlumX Metrics

2006ST13      Nucl.Instrum.Methods Phys.Res. A564, 669 (2006)

J.St-Pierre, G.Kennedy

Re-measurement of Q₀ and k₀ values for 14 nuclides

NUCLEAR REACTIONS ⁷⁵As, ⁸⁷Rb, ⁸⁴Sr, ¹⁰⁸Pd, ¹⁰⁹Ag, ¹¹⁴Cd, ¹¹⁵In, ¹²⁷I, ¹³³Cs, ¹³⁰Ba, ¹⁶⁹Tm, ¹⁸¹Ta, ¹⁸⁵Re(n, γ), E=reactor; measured ratio of resonance integral to thermal neutron activation σ, k₀ values. Two-channel method, comparison with previous results.

doi: 10.1016/j.nima.2006.04.019
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14111.

1995KE16      J.Radioanal.Nucl.Chem. 193, 239 (1995)

G.Kennedy

A Software Counting Loss Correction Method for Neutron Activation Analysis with Short-Lived Radionuclides

RADIOACTIVITY ⁶⁵Zn(EC), (β⁺); ¹³⁷Cs(β^-); measured peak broadening features. ²⁸Al(β^-); measured high energy γ-ray associated deadtime vs count rate. ¹³⁹Ba(β^-); measured low energy γ-ray associated deadtime vs count rate. ^77mSe(IT); ⁵¹Ti(β^-); ⁸⁰Br(β^-), (EC), (β⁺); ²⁷Mg(β^-); ⁶⁶Cu(β^-); ⁵²V(β^-); ⁴⁹Ca(β^-); ³⁸Cl(β^-); ²⁸Al(β^-); measured k parameter for typical γ rays. Software counting loss correction method.

doi: 10.1007/BF02039880
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1990KE08      Nucl.Instrum.Methods Phys.Res. A299, 349 (1990)

G.Kennedy

Comparison of Photopeak Integration Methods

RADIOACTIVITY ¹³⁷Cs; measured photopeak area. Compton background from ⁶⁰Co source, several calculational procedures.

doi: 10.1016/0168-9002(90)90804-F
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1984KE14      Nucl.Instrum.Methods 224, 207 (1984)

G.Kennedy

A Dead-Time Correction Method for Short-Lived Radioisotopes using Measured Peak Areas

RADIOACTIVITY ¹³⁹Ba; ⁵¹Ti; ¹²⁵Sn; ⁸⁷Sr; ⁶⁴Cu; ⁸⁰Br; ²⁷Mg; ⁶⁶Cu; ^28,29Al; ⁴¹Ar; ²⁴Na; ⁵²V; ⁴²K; ²⁰F; ³⁸Cl; ⁵⁶Mn; ⁴⁹Ca; ³⁷S; measured Eγ, Iγ; deduced dead-time to peak count ratio vs source to detector distance. Computer based method.

doi: 10.1016/0167-5087(84)90468-X
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1978JE01      Nucl.Phys. A312, 43 (1978)

H.Jeremie, L.Lemay, M.Irshad, G.Kennedy

The ⁹Be(p, pn)⁸Be (g.s.) Reaction between 10 and 24 MeV

NUCLEAR REACTIONS ⁹Be(p, pn), E=10-24 MeV; measured σ(Ep, θ(p), θ(n)) in kinematically complete geometry; deduced reaction mechanism. ⁹Be deduced level. Natural target.

doi: 10.1016/0375-9474(78)90574-2
Citations: PlumX Metrics

1977JE01      Can.J.Phys. 55, 261 (1977)

H.Jeremie, G.Kennedy

Asymmetric Excitation of the Isobaric Doublet ⁹Be-⁹B Through the ⁹Be(p, pn)⁸Be(gs) Reaction

NUCLEAR REACTIONS ⁹Be(p, pn), E=12.7 MeV; measured σ(Ep, θ), En.

1977KE03      Phys.Rev. C15, 792 (1977)

G.G.Kennedy, J.Deslauriers, S.C.Gujrathi, S.K.Mark

Structure of ¹⁴¹Pm from Decay of N = 79 ¹⁴¹Sm

RADIOACTIVITY ^141m,141Sm; measured Eγ, Iγ, T_1/2, I(ce), Eβ⁺, γγ-, βγ-coin, βγ(t); deduced Q, log ft. ¹⁴¹Pm deduced levels, J, π, T_1/2, ICC, B(λ). Enriched targets, Ge(Li), Si(Li), plastic detectors.

doi: 10.1103/PhysRevC.15.792
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1976KE01      Z.Phys. A276, 103 (1976)

G.G.Kennedy, S.C.Gujrathi, S.K.Mark

The Second 2⁺ State in ¹⁴⁴Sm and the Decay of ¹⁴⁴Eu

RADIOACTIVITY ¹⁴⁴Eu [from ¹⁴⁴Sm(p, n), E=14 MeV]; measured Eγ, Iγ, γγ-coin, T_1/2; deduced log ft. ¹⁴⁴Sm deduced levels.

doi: 10.1007/BF01437704
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1976KE06      Z.Phys. A279, 395 (1976)

G.G.Kennedy, J.Deslauriers, S.C.Gujrathi, S.K.Mark

Search for a 11/2^- → 3/2⁺ M4 Transition in ¹⁴¹Sm

RADIOACTIVITY ^141mSm; measured I(ce), X-ray-ce-coin, K/L ratio, Eγ; deduced EC branching. ¹⁴¹Pm deduced transition, λ.

doi: 10.1007/BF01418135
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1975KE08      Phys.Rev. C12, 553 (1975)

G.G.Kennedy, S.C.Gujrathi, S.K.Mark

Structure of ¹⁴²Sm from the Decay of ¹⁴²Eu

RADIOACTIVITY ^142m,142Eu [from ¹⁴⁴Sm(p, 3n)]; measured Eγ, Iγ, βγ(t), T_1/2, γγ-coin, γ(X-ray)-coin, Eβ; deduced Q(EC), ICC, log ft. ¹⁴²Sm deduced levels, J, π, B(λ), T_1/2.

doi: 10.1103/PhysRevC.12.553
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1975KE09      Z.Phys. A274, 233 (1975)

G.G.Kennedy, S.C.Gujrathi, S.K.Mark

States in N = 80 ¹⁴⁰Nd Populated in the Decay of ¹⁴⁰Pm

RADIOACTIVITY ^140,140mPm; measured T_1/2, Eγ, Iγ, I(ce), γγ-coin; deduced Q, ICC, log ft, J, π. ¹⁴⁰Nd deduced levels, J, π, B(λ).

doi: 10.1007/BF01437735
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1974KE07      Can.J.Phys. 52, 847 (1974)

G.Kennedy, S.C.Gujrathi, P.F.Hinrichsen

Decay of ¹⁴³Eu

RADIOACTIVITY ¹⁴³Eu; measured T_1/2, Eγ, Iγ, γγ-coin; deduced J, β-branching. ¹⁴³Sm deduced levels, J, π.

doi: 10.1139/p74-115
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1973HI01      Nucl.Phys. A212, 365 (1973)

P.F.Hinrichsen, G.Kennedy, T.Paradellis

Level Structure of ⁷⁸Se

RADIOACTIVITY ⁷⁸Br; measured Eγ, Iγ, T_1/2. Deduced logft. ⁷⁸Se deduced levels, J, π.

NUCLEAR REACTIONS ⁷⁸Se(p, p'), E=10 MeV; measured σ(Ep'). ⁷⁸Se deduced levels.

doi: 10.1016/0375-9474(73)90569-1
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Note: The following list of authors and aliases matches the search parameter G.Kennedy: , G.G.KENNEDY