“…A level 2191.93(22) keV is observed on the basis of one populating and one depopulating transition. The prior β-decay study [8] places a 138.5 keV transition, with intensity 7.0(20), tentatively depopulating a level at 3349 keV. Our coincidence data find a 138.05(8) keV transition with intensity 6.5(9) as depopulating a new level at 2192 keV.…”
Section: Experiments and Resultsmentioning
confidence: 54%
“…[10]. Figure 2 highlights the levels observed below 2500 keV as deduced in this work, including a comparison with the previously reported β-decay level scheme [8]. Changes to the level scheme below 2400 keV are discussed in detail below.…”
Section: Experiments and Resultsmentioning
confidence: 90%
“…[7]. Due to the high statistics, the lowest measurable transition intensity was reduced by more than an order of magnitude from the previous ∼0.5 γ rays per 100 decays [8] to ∼0.02 per 100 decays.…”
γ -ray spectroscopy of 132 Te, obtained from β − decay of a 132 Sb radioactive beam at the Holifield Radioactive Ion Beam Facility, was performed using the Clarion array. A significantly revised γ -decay scheme for 132 Te was obtained including a number of new, likely 2 + , states below 2.5 MeV and the removal of a 3 − state at 2280 keV. A simple shell-model interpretation is discussed for the low-lying levels.
“…A level 2191.93(22) keV is observed on the basis of one populating and one depopulating transition. The prior β-decay study [8] places a 138.5 keV transition, with intensity 7.0(20), tentatively depopulating a level at 3349 keV. Our coincidence data find a 138.05(8) keV transition with intensity 6.5(9) as depopulating a new level at 2192 keV.…”
Section: Experiments and Resultsmentioning
confidence: 54%
“…[10]. Figure 2 highlights the levels observed below 2500 keV as deduced in this work, including a comparison with the previously reported β-decay level scheme [8]. Changes to the level scheme below 2400 keV are discussed in detail below.…”
Section: Experiments and Resultsmentioning
confidence: 90%
“…[7]. Due to the high statistics, the lowest measurable transition intensity was reduced by more than an order of magnitude from the previous ∼0.5 γ rays per 100 decays [8] to ∼0.02 per 100 decays.…”
γ -ray spectroscopy of 132 Te, obtained from β − decay of a 132 Sb radioactive beam at the Holifield Radioactive Ion Beam Facility, was performed using the Clarion array. A significantly revised γ -decay scheme for 132 Te was obtained including a number of new, likely 2 + , states below 2.5 MeV and the removal of a 3 − state at 2280 keV. A simple shell-model interpretation is discussed for the low-lying levels.
“…9. The data were taken from the following sources: [35] for 13~ [363 for 132I and a34Cs, E37] for 136La and they were supplemented with information from the compilation of Lederer et al [31] when possible. For ~SSpr, the data were taken from E38] and the excitation energy of the 7-state was deduced to be 0.36___0.02 MeV.…”
The structure of 142Eu is investigated through the beta decay of a42Gd, whose decay half-life is measured to be (69.1 + 1.0) s. A level scheme comprising 42 transitions depopulating 18 excited states is constructed. With the help of the deduced ft values and measured internal conversion coefficients, spin-parity assignments are proposed for several states in 142Eu. The level systematics of the doubly odd, N = 79 isotones are discussed.
“…First level in ~ compared to neighbouring isotopes. The Qp-value of 10 MeV is derived from [18] This branch probably feeds the 931.8 keV level in 96y, leading to a Q~-value of 9~ of: 4 200 _+ 300 keV. Assuming that this beta branch is nearly 100% of the total /~-activity, one obtains log ft,4.…”
9 ~-spectra and half-lives of 9~ 95Rb, 96Rb, 968r, 96y, 132Sb and 132Sn have been measured using the unslowed fission fragment separator "Lohengrin". Preliminary decay schemes for 9~ 95Sr, 96Sr and 96y are given 9
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