Filamentation and surface damage in fused silica with single-mode and multi-mode pulses

We studied filamentation, front surface damage and rear surface damage at 1064 nm and 351 nm with nanosecond pulses on a fused silica optical window. With temporally single-mode pulses, self-focusing occurs together with front surface damage, which is attributed to a Stimulated Brillouin Back Scattering (SBS) wave. The use of temporally multi-mode pulses suppresses the occurrence of front surface damage, and increases self-focusing. With single-mode pulses, the observation of filaments seems coherent with standard Kerr self-focusing effect, and can be understood according to the numerical treatment by Marburger et al, using non linear index values measured in other experiments. However, when multi-mode pulses were used, filaments occurred for much smaller peak intensities, by about a factor of 2. In this case, the non linear index causing self-focusing appears to be twice bigger. This second case is relevant to the situation of vacuum windows in high power laser installations, where the spectrum of light is widened to get rid of SBS. We discuss the physical effects that could be causing the enhancement of self-focusing.

[1]  Edwin L. Kerr Filamentary Tracks Formed in Transparent Optical Glass by Laser Beam Self-Focusing. II. Theoretical Analysis , 1971 .

[2]  Laurent Lamaignère,et al.  Self-focusing and surface damage in fused-silica windows of variable thickness with UV nanosecond pulses , 2004, SPIE Laser Damage.

[3]  Laurent Lamaignere,et al.  Building high-damage-threshold surfaces at 351 nm , 2004, SPIE Optical Systems Design.

[4]  Herve Bercegol,et al.  Growth of damage sites due to platinum inclusions in Nd-doped laser glass irradiated by the beam of a large-scale Nd:glass laser , 2003, SPIE Laser Damage.

[5]  Catherine Pelle,et al.  Wet etching for the mitigation of laser damage growth in fused silica , 2003, SPIE Laser Damage.

[6]  Gerard Raze,et al.  The impact of laser damage on the lifetime of optical components in fusion lasers , 2004, SPIE Laser Damage.

[7]  Patricia Volto,et al.  Self-focusing and rear surface damage in a fused silica window at 1064 nm and 355 nm , 2003, SPIE Laser Damage.

[8]  D. Milam Review and assessment of measured values of the nonlinear refractive-index coefficient of fused silica. , 1998, Applied optics.

[9]  Michael D. Feit,et al.  Growth of laser-initiated damage in fused silica at 351 nm , 2001, SPIE Laser Damage.

[10]  R. B. Wilcox,et al.  Experimental observation and suppression of transverse stimulated Brillouin scattering in large optical components , 1989 .

[11]  Herve Bercegol,et al.  Measurement and prediction of rear surface damage in fused silica windows caused by UV nanosecond pulses , 2005, SPIE Laser Damage.

[12]  David Milam,et al.  Modeling of filamentation damage induced in silica by 351-nm laser pulses , 1997, Laser Damage.

[13]  J. Menapace,et al.  Combined advanced finishing and UV-laser conditioning for producing UV-damage-resistant fused silica optics , 2002 .

[14]  J. H. Marburger,et al.  Computer Studies in Self-Focusing , 1969 .