1992
DOI: 10.1016/0090-3752(92)80043-j
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Nuclear data sheets for A = 132

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Cited by 50 publications
(8 citation statements)
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“…The 5 − 1 state at 2054 keV was previously reported to decay to the 4 + 1 state through a transition of 383 keV [9]. This transition was observed and confirmed to have an intensity consistent with the literature intensity with some reduction in the uncertainty.…”
Section: Experiments and Resultssupporting
confidence: 86%
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“…The 5 − 1 state at 2054 keV was previously reported to decay to the 4 + 1 state through a transition of 383 keV [9]. This transition was observed and confirmed to have an intensity consistent with the literature intensity with some reduction in the uncertainty.…”
Section: Experiments and Resultssupporting
confidence: 86%
“…As a conventional coincidence condition was imposed in the triggering electronics, the experiment provided at most limited sensitivity to coincidences between γ -ray transitions populating and depopulating levels with lifetimes greater than a few microseconds. Thus, coincidences between transitions deexciting the 145-ns isomeric state at 1775 keV [9] and transitions feeding this level could be observed, but no coincidence events were registered between transitions below and above the 1925 keV state (T 1/2 = 28 µs).…”
Section: Experiments and Resultsmentioning
confidence: 72%
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“…Based on these observations and considerations, we safely conclude that the half-life of the first excited state in 132 I is 1.120 ± 0.015 ns. The transition probability, B(M1), was deduced to be 0.024 W.u., from the present half-life value, the internal conversion coefficient α = 5.62, calculated by BrIcc [15], and the fact that the transition is pure M1 [16]. This small B(M1) value may indicate a large M1 retardation for this state.…”
Section: Discussionmentioning
confidence: 92%