Particle damage sources for fused silica optics and their mitigation on high energy laser systems

High energy laser systems are ultimately limited by laser-induced damage to their critical components. This is especially true of damage to critical fused silica optics, which grows rapidly upon exposure to additional laser pulses. Much progress has been made in eliminating damage precursors in as-p...

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Veröffentlicht in:Optics express 2017-05, Vol.25 (10), p.11414-11435
Hauptverfasser: Bude, J, Carr, C W, Miller, P E, Parham, T, Whitman, P, Monticelli, M, Raman, R, Cross, D, Welday, B, Ravizza, F, Suratwala, T, Davis, J, Fischer, M, Hawley, R, Lee, H, Matthews, M, Norton, M, Nostrand, M, VanBlarcom, D, Sommer, S
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Sprache:eng
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Zusammenfassung:High energy laser systems are ultimately limited by laser-induced damage to their critical components. This is especially true of damage to critical fused silica optics, which grows rapidly upon exposure to additional laser pulses. Much progress has been made in eliminating damage precursors in as-processed fused silica optics (the advanced mitigation process, AMP3), and very high damage resistance has been demonstrated in laboratory studies. However, the full potential of these improvements has not yet been realized in actual laser systems. In this work, we explore the importance of additional damage sources-in particular, particle contamination-for fused silica optics fielded in a high-performance laser environment, the National Ignition Facility (NIF) laser system. We demonstrate that the most dangerous sources of particle contamination in a system-level environment are laser-driven particle sources. In the specific case of the NIF laser, we have identified the two important particle sources which account for nearly all the damage observed on AMP3 optics during full laser operation and present mitigations for these particle sources. Finally, with the elimination of these laser-driven particle sources, we demonstrate essentially damage free operation of AMP3 fused silica for ten large optics (a total of 12,000 cm of beam area) for shots from 8.6 J/cm to 9.5 J/cm of 351 nm light (3 ns Gaussian pulse shapes). Potentially many other pulsed high energy laser systems have similar particle sources, and given the insight provided by this study, their identification and elimination should be possible. The mitigations demonstrated here are currently being employed for all large UV silica optics on the National Ignition Facility.
ISSN:1094-4087
1094-4087
DOI:10.1364/OE.25.011414