2018
DOI: 10.1016/j.optlastec.2018.04.014
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Experimental research on temperature field distributions for optical lenses irradiated by femtosecond laser

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Cited by 3 publications
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“…The following electron–phonon scattering process to reach an equilibrium temperature of the electron and phonon system induces an ultrafast phonon heating process (for 28 mJ cm −2 laser fluence, the maximum temperature rise is 22.6 K) with a heating rate of >10 13 K s −1 in hundreds of femtoseconds (see the Supplementary material for theoretical analysis of temperature rise by PiP) and an ultrafast thermal gradient with the Gaussian distribution is generated in the focus zone ( Supplementary Fig. S1a ) [ 24 ]. On the way to cooling the excited system, atoms obtain excessive kinetic energy to align into an ordered arrangement, thus passivating the bulk defects of the SnO 2 and improving the crystallinity of the SnO 2 [ 21 , 25 ].…”
Section: Resultsmentioning
confidence: 99%
“…The following electron–phonon scattering process to reach an equilibrium temperature of the electron and phonon system induces an ultrafast phonon heating process (for 28 mJ cm −2 laser fluence, the maximum temperature rise is 22.6 K) with a heating rate of >10 13 K s −1 in hundreds of femtoseconds (see the Supplementary material for theoretical analysis of temperature rise by PiP) and an ultrafast thermal gradient with the Gaussian distribution is generated in the focus zone ( Supplementary Fig. S1a ) [ 24 ]. On the way to cooling the excited system, atoms obtain excessive kinetic energy to align into an ordered arrangement, thus passivating the bulk defects of the SnO 2 and improving the crystallinity of the SnO 2 [ 21 , 25 ].…”
Section: Resultsmentioning
confidence: 99%