Fig. 2 Characterization of fs-laser–induced degradation.

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Presentation transcript:

Fig. 2 Characterization of fs-laser–induced degradation. Characterization of fs-laser–induced degradation. (A to C) The change on the surface of red HgS powder after excessive exposure to fs-laser power. All images were taken under identical conditions (720 and 817 nm, 0.45/0.45 mW, τ = 60 fs). (A) The initial status of red HgS. (B) The surface changes after inducing degradation at powers of 0.45/0.90 mW. (C) After inducing further degradation at powers of 0.45/0.9 and 0.9/0.9 mW. (D) XRD spectra of red, black, and degraded red HgS powder for angles near 30.5°. (E) EDS spectra of the same samples (signals were normalized by photon counts at 2.309 eV; see fig. S4 for the corresponding SEM images). All samples show similar Hg and S peak intensities at 2.195 (Hg, Mα), 2.281 (Hg, Mβ), 2.309 (S, Kα), and 2.465 eV (S, Kβ) and show a negligible amount of Cl peak intensities at 2.622 eV (Cl, Kα). (F) Occurrence of a positive ESA signal in regions that turn from α- to β-HgS. Signals were extracted from the fixed ROI [marked in (A) to (C)] of a series of images acquired at different power levels (the number in parenthesis indicates the order of acquisition, followed by the power levels). Jin Yu et al. Sci Adv 2019;5:eaaw3136 Copyright © 2019 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).