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NSR database version of May 8, 2024.

Search: Author = R.K.Heaton

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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.