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Y. Shigekawa

Publications and source records attributed to Y. Shigekawa.

3 recordsLinked to original sources

Chemical effects on nuclear decay of $^{235}$U isomer in the uranyl form

The nucleus of uranium-235 ($^{235}$U) possesses an exceptionally low-energy isomeric state, $^{235m}$U. Unlike most radioactive nuclides, whose nuclear-decay half-lives are constant, the half-life of $^{235m}$U varies with its chemical environment$^{1,2}$ owing to interactions with outer-shell electrons in the internal-conversion (IC) process. However, the mechanism underlying this half-life variation, particularly the role of molecular bonding beyond simple electron-density effects$^{1,2}$, remains unresolved. Here, we investigate variations in the half-lives of $^{235m}$U and the corresponding IC-electron energy spectra for uranyl (UO2$^{2+}$) compounds with different halide ligands. The half-lives of $^{235m}$U are measured to be 25.32(4), 26.05(8), 25.84(3), and 25.44(3) min for uranyl fluoride, chloride, bromide, and iodide, respectively, indicating that the half-life increases with increasing ligand electronegativity, with the exception of uranyl fluoride. The shortest half-life observed for uranyl fluoride is attributed to the smallest number of 6p electrons occupying bonding orbitals, as indicated by the IC-electron energy spectra and quantum chemical calculations. This work provides the first observation of a significant variation in a nuclear decay process driven by changes in molecular orbital formation, paving the way toward a deeper understanding of interactions between a nucleus and electrons involved in chemical bonding.

nucl-ex

Estimation of radiative half-life of $^{229m}$Th by half-life measurement of other nuclear excited states in $^{229}$Th

We perform coincidence measurements between $α$ particles and $γ$ rays from a $^{233}$U source to determine the half-lives of the excited state in a $^{229}$Th nucleus. We first prove that the half-lives of 42.43- and 164.53-keV states are consistent with literature values, whereas that of the 97.14-keV state (93(7) ps) deviates from a previously measured value (147(12) ps). The half-lives of 71.83- and 163.25-keV states are determined for the first time. Based on the obtained half-lives and the Alaga rule, we estimate the radiative half-life of the low-energy isomeric state ($^{229m}$Th) to be $5.0(11)\times10^{3}$ s, which is one of the key parameters for the frequency standard based on $^{229}$Th.

nucl-ex

Nuclear resonant scattering experiment with fast time response: new scheme for observation of $^{229\rm m}$Th radiative decay

Nuclear resonant excitation of the 29.19-keV level in $^{229}$Th with high-brilliance synchrotron- radiation and detection of its decay signal, are proposed with the aim of populating the extremely low-energy isomeric state of $^{229}$Th.The proposed experiment, known as nuclear resonant scattering (NRS), has the merit of being free from uncertainties about the isomer level energy. However, it requires higher time resolution and shorter tail in the response function of the detector than that of conventional NRS experiments because of the short lifetime of the 29.19-keV state. We have fabricated an X-ray detector system which has a time resolution of 56 ps and a shorter tail function than the previously reported one. We have demonstrated an NRS experiment with the 26.27-keV nuclear level of $^{201}$Hg for feasibility assessment of the $^{229}$Th experiment. The NRS signal is clearly distinct from the prompt electronic scattering signal by the implemented detector system. The half-life of the 26.27-keV state of $^{201}$Hg is determined as 629 $\pm$ 18 ps which is better precision by a factor three than that reported to date.

nucl-ex