1972
DOI: 10.1002/pssb.2220490204
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Self‐diffusion of cesium‐134 and diffusion of rubidium‐86 in cesium iodide single crystals

Abstract: The self-diffusion of Cs-134 and the diffusion of Rb-86 in CsI single crystals were measured in the temperature range 404 t.0 603 "C using the tracer-sectioning technique. The temperature dependencies of diffusion coefficients are D = (17.6fi::) exp [-(35400 * 140)/RT] om2 8-1 for 0 -1 3 4 and D = (27.3?2$') exp [-(34540 It 160)/RT] cm2 s-l for Rb-86. Comparison of present data with earlier results on diffusion parameters of Na-22 in CsI single crystals shows that there is 110 dependence of the activation ener… Show more

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Cited by 11 publications
(1 citation statement)
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“…Furthermore, the greater covalent nature of the Tl-I bond will also increase the activation energy for Tl to diffuse in the CsI lattice. These arguments are consistent with the published data [27] where Na has the highest diffusion coefficient ( , diffusion coefficient at infinite temperature or pre-exponential diffusion coefficient) and the lowest activation energy in comparison to Cs, Rb and K in CsI crystals. Furthermore, the ripening process observed in the CsI thick films [11] demonstrates that Na can be quite mobile in the CsI lattice at room temperature.…”
Section: Materials Characterizationsupporting
confidence: 93%
“…Furthermore, the greater covalent nature of the Tl-I bond will also increase the activation energy for Tl to diffuse in the CsI lattice. These arguments are consistent with the published data [27] where Na has the highest diffusion coefficient ( , diffusion coefficient at infinite temperature or pre-exponential diffusion coefficient) and the lowest activation energy in comparison to Cs, Rb and K in CsI crystals. Furthermore, the ripening process observed in the CsI thick films [11] demonstrates that Na can be quite mobile in the CsI lattice at room temperature.…”
Section: Materials Characterizationsupporting
confidence: 93%