Atom Motion in Solids Following Nuclear Transmutation

G. Collins
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Abstract

Following nuclear decay, a daughter atom in a solid will "stay in place" if the recoil energy is less than the threshold for displacement. At high temperature, it may subsequently undergo long-range diffusion or some other kind of atomic motion. In this paper, motion of 111Cd tracer probe atoms is reconsidered following electron-capture decay of 111In in the series of In3R phases (R= rare-earth). The motion produces nuclear relaxation that was measured using the method of perturbed angular correlation. Previous measurements along the entire series of In3R phases appeared to show a crossover between two diffusional regimes. While relaxation for R= Lu-Tb is consistent with a simple vacancy diffusion mechanism, relaxation for R= Nd-La is not. More recent measurements in Pd3R phases demonstrate that the site-preference of the parent In-probe changes along the series and suggests that the same behavior occurs for daughter Cd-probes. The anomalous motion observed for R= Nd-La is attributed to "lanthanide expansion" occurring towards La end-member phases. For In3La, the Cd-tracer is found to jump away from its original location on the In-sublattice in an extremely short time, of order 0.5 ns at 1000 K and 1.2 ms at room temperature, a residence time too short to be consistent with defect-mediated diffusion. Several scenarios that can explain the relaxation are presented based on the hypothesis that daughter Cd-probes first jump to neighboring interstitial sites and then are either trapped and immobilized, undergo long-range diffusion, or persist in a localized motion in a cage.
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核嬗变后固体中的原子运动
在核衰变之后,如果反冲能量小于位移阈值,固体中的子原子将“留在原地”。在高温下,它可能随后进行远距离扩散或某种其他类型的原子运动。本文重新考虑了111Cd示踪探针原子在In3R相(R=稀土)系列中111In的电子俘获衰变后的运动。这种运动产生的核弛豫是用摄动角相关法测量的。先前沿着整个In3R相系列的测量似乎显示了两种扩散状态之间的交叉。R= Lu-Tb的弛豫符合简单的空位扩散机制,而R= Nd-La的弛豫则不符合。最近对Pd3R相的测量表明,父探针的位置偏好沿着系列发生变化,并且表明子探针也会发生相同的行为。观察到的R= Nd-La的异常运动归因于“镧系元素膨胀”发生在La端元相。对于In3La,发现cd示踪剂在极短的时间内从in -亚晶格上的原始位置跳离,在1000 K时为0.5 ns,在室温下为1.2 ms,停留时间太短,无法与缺陷介导的扩散相一致。基于以下假设,提出了几种可以解释弛豫的情况:子cd探针首先跃迁到邻近的间隙点,然后要么被困住并固定,要么进行远程扩散,要么在笼子里保持局部运动。
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