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NSR database version of April 11, 2024.

Search: Author = R.K.Heaton

Found 2 matches.

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1997HE11      Phys.Rev. C56, 922 (1997)

R.K.Heaton, H.W.Lee, B.C.Robertson, E.B.Norman, K.T.Lesko, B.Sur

α-Particle Induced γ-Ray Transitions in Light Elements

NUCLEAR REACTIONS, ICPND 10B(α, p), (α, d), E=5.6-10 MeV; 11B(α, n), E=5.6-10 MeV; 19F(α, α'), (α, p), E=5.6-10 MeV; 23Na(α, n), (α, p), E=5.6-10 MeV; 24Mg(α, p), 25Mg(α, α'), (α, n), E ≤ 10 MeV; 26Mg(α, n), (α, p), E=5.6-10 MeV; 27Al(α, α'), E=10 MeV; 27Al(α, n), E=7-10 MeV; 27Al(α, p), E=5.6-10 MeV; 28Si(α, p), 29,30Si(α, n), (α, p), E=10 MeV; measured thick target residuals yields; deduced reaction mechanism related features. 28,29,30Si deduced excitation distribution vs Eα. Comparison of several models.

doi: 10.1103/PhysRevC.56.922
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0495.


1995HE40      Nucl.Instrum.Methods Phys.Res. A364, 317 (1995)

R.K.Heaton, H.W.Lee, B.C.Robertson, E.B.Norman, K.T.Lesko, B.Sur

α-Particle Induced High-Energy γ-Ray Yields from Light Elements

NUCLEAR REACTIONS, ICPND 27Al, 24Mg, 10B, 19F(α, p), 10B(α, d), 11B, 19F, 25,26Mg, 27Al(α, n), E=5.6-10 MeV; measured thick target γ yields; deduced γ production intensity distributions from materials related features. Thick targets of Be also studied.

doi: 10.1016/0168-9002(95)00220-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0495.


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