Low Excited States in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">Li</mml:mi></mml:mrow><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">Be</mml:mi></mml:mrow><mml:mrow><mml:mn>9</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>

Browne, C.P.; Williamson, R. M.; Craig, D.S.; Donahue, D. J.

doi:10.1103/physrev.83.179

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Cited by 33 publications

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“…For partially polarized 7-radiation, the coincidence counting rate ratio has a value intermediate between unity and the value for plane polarized radiation. A detailed calculation by Steenberg 6 and Tolhoek and Cox 7 shows that the counting ratio increases from unity to its limiting value as the nuclear alignment becomes more and more complete. The limiting value for complete alignment is greatest for radiation emitted along the b axis (along which we observed).…”

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confidence: 99%