Refine your search:     
Report No.
 - 
Search Results: Records 1-1 displayed on this page of 1
  • 1

Presentation/Publication Type

Initialising ...

Refine

Journal/Book Title

Initialising ...

Meeting title

Initialising ...

First Author

Initialising ...

Keyword

Initialising ...

Language

Initialising ...

Publication Year

Initialising ...

Held year of conference

Initialising ...

Save select records

Journal Articles

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*; et al.

RIKEN Accelerator Progress Report, Vol.46, P. 237, 2013/00

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.

1 (Records 1-1 displayed on this page)
  • 1