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Oral presentation

First ionization potentials of the heaviest elements

Nagame, Yuichiro

no journal, , 

Oral presentation

Fine-structure $$alpha$$-decay spectroscopy of superheavy nuclei

Asai, Masato

no journal, , 

To investigate nuclear structure of superheavy nuclei experimentally, spectroscopic methods which can reveal level structure of ground- and excited states are the most effective. In particular, fine-structure $$alpha$$-decay spectroscopy is expected to be a very sensitive method because spectroscopic information can be obtained only through $$alpha$$-particle measurements. However, it is difficult to measure $$alpha$$ particles of superheavy nuclei with high energy resolution. Moreover, the observed $$alpha$$ energy spectra are significantly distorted by coincidence summing effects. I would like to demonstrate how we can overcome these difficulties, and how useful the fine-structure $$alpha$$-decay spectroscopy is to investigate nuclear structure of superheavy nuclei.

Oral presentation

Adsorption behavior of lawrencium on a tantalum surface

Sato, Tetsuya; Kaneya, Yusuke*; Asai, Masato; Tsukada, Kazuaki; Toyoshima, Atsushi; Mitsukai, Akina*; Osa, Akihiko; Makii, Hiroyuki; Hirose, Kentaro; Nagame, Yuichiro; et al.

no journal, , 

Our experimental results on the first ionization potential measurement of lawrencium (Lr, element 103) have strongly suggested that the Lr atom has a [Rn]$$7s^25f^{14}7p_{1/2}$$ configuration as a result of the influence of strong relativistic effects. The configuration is different from that expected from the lanthanide homologue, lutetium (Lu). According to a semi-empirical consideration, it is expected that the change of the electronic configuration leads higher volatility of Lr than that of Lu. In this work, adsorption behaviors of Lr and various short-lived rare earth isotopes on a tantalum surface were investigated via observation of their surface ionization efficiencies. It was found that Lr would behave like low volatile rare earth elements such as Lu contrary to the semi-empirical expectation.

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