2010
DOI: 10.1140/epja/i2010-10958-2
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Precise half-life measurements for 38Ca and 39Ca

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Cited by 20 publications
(13 citation statements)
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“…These were each obtained by observation and analysis of the decay of β-delayed γ-rays from the daughter, 38 K. The first result lies about one-and-a-half of its error bar away from our quoted half-life; the other three agree well within their error bars. There is a much more recent measured value, 443.8(19) ms [8], which was obtained in a similar manner to ours, from a measurement of the decay positrons in a gas counter; in their case, though, sample purity was achieved by collecting the 38 Ca first in a Penning trap. Our half-life result agrees well with theirs but with an uncertainty five times smaller.…”
Section: F Comparison With Previous Resultssupporting
confidence: 73%
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“…These were each obtained by observation and analysis of the decay of β-delayed γ-rays from the daughter, 38 K. The first result lies about one-and-a-half of its error bar away from our quoted half-life; the other three agree well within their error bars. There is a much more recent measured value, 443.8(19) ms [8], which was obtained in a similar manner to ours, from a measurement of the decay positrons in a gas counter; in their case, though, sample purity was achieved by collecting the 38 Ca first in a Penning trap. Our half-life result agrees well with theirs but with an uncertainty five times smaller.…”
Section: F Comparison With Previous Resultssupporting
confidence: 73%
“…The value of Q EC is used to determine the statistical rate function, f , while t 1/2 and R are combined to obtain the partial half-life, t. Before our half-life measurement of 38 Ca, which is reported here, only its Q EC value was known to the desired precision: it had been measured with Penning-traps to ±0.006% [5][6][7], which corresponds to an f -value precision of ±0.03% [2]. The most precise half-life result was only known to ±0.4% [8] and the superallowed branching ratio has not yet been measured at all.…”
mentioning
confidence: 99%
“…V B convincingly rule out the possibility of large numbers of unobserved weak transitions to higher excited states that sum to appreciable strength -the Pandemonium effect [24,25] -so we can safely conclude that the Gamow-Teller sum we have obtained accounts for all the non-superallowed strength in the decay of 38 Ca. The branching ratio for the superallowed 0 + → 0 + transition to the 130-keV analog state is thus 0.7728 (16), a result we obtain simply by subtracting the total GamowTeller branching ratio from unity. Note that, as we do so, we convert the relative precision of our measurement, which is 0.70% (= 0.0016/0.2272), to a relative precision of 0.21% (= 0.0016/0.7728) for the quantity we have sought to obtain: the superallowed branching ratio.…”
Section: B Branching Ratio For the Superallowed Transitionmentioning
confidence: 86%
“…The total branching ratio for all five Gamow-Teller transitions -to the 1 + states at 459, 1698, 3341, 3856 and 3977 keV -is 0.2272 (16). This is simply the sum of the corresponding branching ratios in column six of Table V.…”
Section: B Branching Ratio For the Superallowed Transitionmentioning
confidence: 93%
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