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Development of high-power laser coatings
Laser resistance and stress-free mirrors, windows, polarizers, and beam splitters up to $400~\mathrm{mm} \times 400~\mathrm{mm} $ are required for the construction of the series SG facilities. In order to improve the coating quality, a program has been in place for the last ten years. For the small-...
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Published in: | High power laser science and engineering 2013-03, Vol.1 (1), p.36-43 |
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Main Authors: | , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Laser resistance and stress-free mirrors, windows, polarizers, and beam splitters up to
$400~\mathrm{mm} \times 400~\mathrm{mm} $
are required for the construction of the series SG facilities. In order to improve the coating quality, a program has been in place for the last ten years. For the small-aperture pick-off mirror, the laser-induced damage threshold (LIDT) is above
$60~\mathrm{J} / {\mathrm{cm} }^{2} $
(1064 nm, 3 ns), and the reflected wavefront is less than
$\lambda / 4~(\lambda = 633~\mathrm{nm} )$
. The Brewster-angle polarizing beam splitter (
$\Phi 50\times 10~\mathrm{mm} $
) shows the best LIDT result, up to
$29. 8~\mathrm{J} ~{\mathrm{cm} }^{- 2} $
(1064 nm, 10 ns) for a p-polarized wave in the 2012 damage competition of the XLIV Annual Boulder Damage Symposium. For the larger-aperture mirror and polarizer, the LIDT is above
$23~\mathrm{J} ~{\mathrm{cm} }^{- 2} $
(1064 nm, 3 ns) and
$14~\mathrm{J} ~{\mathrm{cm} }^{- 2} $
(1064 nm, 3 ns), respectively. The reflected wavefront is less than
$\lambda / 3~(\lambda = 633~\mathrm{nm} )$
at the used angle. |
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ISSN: | 2095-4719 2052-3289 |
DOI: | 10.1017/hpl.2013.6 |