首页> 外文期刊>Radiochimica Acta: International Journal for Chemical Aspects of Nuclear Science and Technology >Production of ~(256)Lr in the ~(249,250,251)Cf + ~(11)B, ~(243)Am + ~(18)O, and ~(248)Cm + ~(14)N reactions
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Production of ~(256)Lr in the ~(249,250,251)Cf + ~(11)B, ~(243)Am + ~(18)O, and ~(248)Cm + ~(14)N reactions

机译:〜(249,250,251)Cf +〜(11)B,〜(243)Am +〜(18)O和〜(248)Cm +〜(14)N反应生成〜(256)Lr

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摘要

Production cross-sections of the isotope ~(256)Lr in the ~(249,250,251)Cf +~(11)B, ~(243)Am+~(18)O, and ~(248)Cm+~(14)N reactions were measured using a He/KCl gas-jet transport system and a rotating wheel α-particle detection apparatus. The α-particle energy of ~(256)Lr was distributed from 8.3 to 8.7MeVand its half-life, T_(1/2),was measured to be 28±1 s. The maximum cross sections in the ~(249)Cf (~(11)B, 4n)~(256)Lr and ~(243)Am(~(18)O, 5n)~(256)Lr reactions were determined to be 122 ± 36 nb at the beam energy of 63MeV and 26 ± 7 nb at 96MeV, respectively. In the ~(248)Cm(~(14)N, 6n)~(256)Lr reaction, the cross section was measured to be 27 ± 10 nb at 91MeV.
机译:〜(249,250,251)Cf +〜(11)B,〜(243)Am +〜(18)O和〜(248)Cm +〜(14)N反应中的同位素〜(256)Lr的生产截面为使用He / KCl喷气传输系统和旋转轮α粒子检测设备进行测量。 〜(256)Lr的α粒子能量分布在8.3MeV至8.7MeV之间,其半衰期T_(1/2)为28±1 s。确定〜(249)Cf(〜(11)B,4n)〜(256)Lr和〜(243)Am(〜(18)O,5n)〜(256)Lr反应的最大截面为光束能量为63MeV时为122±36 nb,96MeV为26±7 nb。在〜(248)Cm(〜(14)N,6n)〜(256)Lr反应中,在91MeV下测得的截面为27±10 nb。

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