<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Cl</mml:mi></mml:mrow><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>37</mml:mn></mml:mrow><mml:mrow /><mml:mrow /></mml:mmultiscripts></mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">He</mml:mi></mml:mrow><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow /><mml:mrow /></mml:mmultiscripts

Corwin, William C.; Segel, R. E.

doi:10.1103/physrevc.15.505

Cited by 8 publications

(1 citation statement)

References 10 publications

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“…The other selectively populated states are reached by ℓ = 4, 6, or a mixture of 4 and 6. In contrast, the 37 Cl( 3 He,p) reaction [9] shows a very different selectivity even though it transfers the same proton plus neutron combination. This reaction favors low-spin states and the most strongly populated one is the 3/2 + isobaric analog of the g.s.…”

Section: Introductionmentioning

confidence: 96%

High spin structure of Ar39 and the FSU cross-shell interaction

et al. 2019

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High-spin states in 39 Ar were populated using the 27 Al(14 C, pn) reaction at 25.6 MeV. The deexciting γ rays were measured with the FSU γ detector array along with evaporation protons in a Si E-∆E telescope. The known high-spin level scheme was extended up to over 11 MeV with a dozen new levels above the neutron decay threshold. The decay pattern appears somewhat atypical for heavy-ion fusion-evaporation reactions. The structure of 39 Ar is discussed in terms of the new FSU cross-shell spsdpf interaction fitted to a wide range of nuclei. This interaction has proved quite successful in accounting for the level scheme of 39 Ar, including the previously suggested fully aligned πf 7/2 ⊗ νf 7/2 17/2 + state and previously discovered analogs of the lowest states in 39 Cl.

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Section: Introductionmentioning

confidence: 96%