2011
DOI: 10.1103/physrevb.84.245103
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Time-resolved plasma measurements in Ge-doped silica exposed to infrared femtosecond laser

Abstract: Document VersionPublisher's PDF, also known as Version of Record (includes final page, issue and volume numbers)Please check the document version of this publication:• A submitted manuscript is the author's version of the article upon submission and before peer-review. There can be important differences between the submitted version and the official published version of record. People interested in the research are advised to contact the author for the final version of the publication, or visit the DOI to the … Show more

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Cited by 20 publications
(13 citation statements)
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“…As a result no apparent structural change could be observed. Besides, due to the short plasma lifetime of ~150 fs in SiO 2 glass , the following formation mechanisms of nanogratings are proposed: the non‐radiative relaxation of excitons via relative long lifetime transition from self‐trapped excitons (STE) to point‐defecs (their lifetime is several hundred picoseconds at room temperature) . In particular, a common feature of periodic nanostructure formation between c‐Si and SiO 2 glass is the existence of a transition with a long relaxation time.…”
Section: Methodsmentioning
confidence: 99%
“…As a result no apparent structural change could be observed. Besides, due to the short plasma lifetime of ~150 fs in SiO 2 glass , the following formation mechanisms of nanogratings are proposed: the non‐radiative relaxation of excitons via relative long lifetime transition from self‐trapped excitons (STE) to point‐defecs (their lifetime is several hundred picoseconds at room temperature) . In particular, a common feature of periodic nanostructure formation between c‐Si and SiO 2 glass is the existence of a transition with a long relaxation time.…”
Section: Methodsmentioning
confidence: 99%
“…In this case, the phase transition process is considered to take place due to high-repetition-rate fs-laserinduced heat accumulation. The electronic excitation is initiated by multiphoton ionization [12], and subsequent electron-phonon coupling leads to temperature increase. Then at high repetition rate (typ.…”
Section: Introductionmentioning
confidence: 99%
“…Additionally, two intense absorption bands can be distinguished at short wavelengths, which are attributed to SiE' centers at 210 nm (≡Si, an unpaired electron in a silicon atom bound to three oxygen atoms), and oxygen deficiency center (ODC)(II) at 245 nm, (-O-Si-O-, a divalent silicon atom) [27,28]. A detailed description of their formation mechanism is given in [29]. In addition the absorption measurements of the sample after annealing at 600 °C for 2 h clearly indicated complete erasure of the E' and ODC(II) defects if attributed to the absorption bands observed at 210 and 240 nm, respectively (Figure 5a).…”
Section: Loss and Birefringence Dispersionmentioning
confidence: 99%