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Production of $$^{256}$$Lr in the $$^{248}$$Cm + $$^{14}$$N reaction

Sato, Nozomi; Sato, Tetsuya   ; Asai, Masato  ; Toyoshima, Atsushi; Tsukada, Kazuaki  ; Li, Z.*; Nishio, Katsuhisa   ; Nagame, Yuichiro ; Sch$"a$del, M.; Haba, Hiromitsu*; Ichikawa, Shinichi; Kikunaga, Hidetoshi*

Due to the strong relativistic effects, the weakly-bound outermost electron results in a significantly low first ionization potential (IP) of Lr as compared with its neighboring heavy actinides. The isotope $$^{256}$$Lr, with a relatively long half-life of 27 s, is the suitable candidates for the IP measurement of Lr through the surface ionization method. In the present study, we measured the cross section of the $$^{248}$$Cm($$^{14}$$N, 6$$n$$)$$^{256}$$Lr reaction to evaluate the production rate of $$^{256}$$Lr. A $$^{248}$$Cm target with 960 $$pm$$ 60 $$mu$$g/cm$$^{2}$$ thickness was bombarded with a $$^{14}$$N$$^{5+}$$ beam from the RIKEN AVF Cyclotron. The beam energy was 91 MeV in the middle of the target. The average beam intensity was 1.2 particle-$$mu$$A. Reaction products were transported to the rotating wheel $$alpha$$-particle detection system with a He/KCl gas-jet system. The $$^{256}$$Lr cross section of 27$$pm$$1 nb was calculated based on the $$alpha$$-particle events between 8.3 and 8.7 MeV.

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