Low-lying states in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Ar</mml:mi></mml:mrow><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>39</mml:mn></mml:mrow><mml:mrow /><mml:mrow /></mml:mmultiscripts></mml:mrow></mml:math>from the<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 />

Tonn, J. F.; Segel, R. E.; Corwin, William C.; Rutledge, L. R.

doi:10.1103/physrevc.16.2065

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“…An interesting exception is the (α, d) reaction which preferentially populates higher-spin states, most strongly those in which the spins of the transferred protons and neutrons are fully aligned, as in the deuteron g.s. This is clearly seen in two 37 Cl(α, d) reaction studies [7,8].…”

Section: Introductionmentioning

confidence: 72%

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: 72%