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Figure 6
(a) Probability of occurrence of a radiation-induced defect in the crystal obtained by fitting a Hendricks–Teller model to the time evolution of a (200) Bragg peak. After a latent period, the probability increases linearly with time. (b) Fitted value of the spacing of the radiation-induced defects in the crystal. The values obtained for the spacing during the latent period are unreliable. Once the crystal starts to disintegrate, the fitted value is fairly constant (90 Å) and is about 2 Å below the indicated bulk value for a defect-free crystal (91.5 Å).

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 13| Part 1| December 2006| Pages 1-7
doi:10.1107/S0909049505038811
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