Energies of the Radiations from<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">Co</mml:mi></mml:mrow><mml:mrow><mml:mn>57</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">Co</mml:mi></mml:mrow><mml:mrow><mml:mn>58</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>

Cork, J. M.; Brice, M. K.; Schmid, L.C.

doi:10.1103/physrev.99.703

Cited by 25 publications

(2 citation statements)

References 4 publications

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“…The spectrum is dominated by radiation arising from the EC/β + decay of 58 Co g , along with an easily visible contribution from the decay of 57 Co. The small peak at 1322 keV is due to summing of annihilation radiation with the 810.8-keV photon [43]. The cobalt fraction was radiochemically pure, other than a very small contribution from 3.4-hour 61 Cu [44].…”

Section: Nuclidementioning

confidence: 98%

Decay of Com58

Moody¹,

Gharibyan²,

Grant³

et al. 2019

Phys. Rev. C

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We have studied some of the nuclear decay properties of 58 Co m . The half-life is found to be (8.853 ± 0.023) hours, which is significantly different from the evaluations found in the literature. The absolute intensity of the 24.9-keV γ-ray emitted in the IT decay is (0.0387 ± 0.0016)%, in agreement with the calculated yield of a transition of M 3 multipolarity. We observe γ-ray photons from a previously unreported branch for EC decay, with an intensity of (0.00120 ± 0.00005)%, consistent with expectations from the calculation of log f t.

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Section: Nuclidementioning

confidence: 98%

Decay of Com58

Moody¹,

Gharibyan²,

Grant³

et al. 2019

Phys. Rev. C

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“…1 This provides further support for the Fermi theory of beta decay for allowed transitions. After the exclusion of the nuclides which show particularly low-transition probabilities such as Zn 65 , 2 Co 58 , 3 and those which have the magic number configurations in parent nuclides such as Co 55 , Ni 57 , and Sn 111 ; investigation of regularities in comparative half-lives of the allowed i£-capture transitions has been attempted. (1) The i£-capture for odd nuclides can be classified as either unlike-core or like-core transitions.…”

Section: Longitudinal Photomagnetoelectric Effect In Germaniummentioning

confidence: 99%

Minutes of the Fall Meeting of the Ohio Section of the American Physical Society Held at Wright-Patterson Air Force Base, Ohio, October 14 and 15, 1955

Anonymous

1955

Phys. Rev.

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of the Aeronautical Research Laboratory, we owe our sincere thanks for the opportunity to visit Wright-Patterson Air Force Base and the several laboratories, for the program of tours, overnight accommodation, and the thoughtful care of our smallest needs. It was a large meeting, 72 registered not including men at the Base itself, 21 colleges were represented, 9 corporations having research facilities, and three government research agencies besides the organizations at the Base.On Friday, October 14, Major General Swofford, the Commandant, USAFIT began the program with an over-all picture of military research organizations. Mr. Wendell Koch,

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