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We find that a transition from homogenous to highly localized deformation occurs at a critical loop density.
Loop density and swelling was shown to have similar values in grains sizes that range from 80too 600 nm.
The results demonstrate a strong correlation between the dislocation loop density and areal coverage, and the light emission efficiency.
The faulted loop density increased with dose from 1 dpa up to 10 dpa where it saturated and remained approximately the same until 20 dpa.
The structural properties, including the epoxide conversion, the weight average molecular weight, the sol gel fraction, the number average branch point of the sol part, the branch as well as the loop density of the gel part were discussed.
Increase in dislocation loop density was shown to provide the dominant contribution to radiation hardening at the late irradiation stages (after reaching double the design end-of-life neutron fluence of ∼4 × 1024 n m−2).
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The HSP101 NBD2 pore loop densities are coloured by HSP101 protomer, and the cargo density is coloured pink.
The loop number density varied between 1022 and 1023 loops/m3.
Further, MicroViBe enables consistent, objective quantitative approximation of the b = ½ <111> dislocation loop number density.
Under the same irradiation conditions, loop number densities in the W-Re and W-Ta alloys were higher than in pure W but loops were smaller.
In particular, we show that the high loop column densities inferred from the GOES and RHESSI soft X-ray emeasure meandre and the volume of the flare loop are consistent with the coronal thick-target interpretation of the HXR images and spectra.
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