Optomechanical Coatings for High-Power Mirrors and Adaptive Optics

2009 ◽  
Author(s):  
Joseph J. Talghader
Keyword(s):  
Author(s):  
B. Parry ◽  
A. Boyle ◽  
M. Galimberti ◽  
C. Hooker ◽  
L. Walker ◽  
...  

2016 ◽  
Vol 05 (02) ◽  
pp. 1650001 ◽  
Author(s):  
Angel Otarola ◽  
Paul Hickson ◽  
Ronald Gagné ◽  
Yong Bo ◽  
Junwei Zuo ◽  
...  

We present results of on-sky tests performed in the summer of 2013 to characterize the performance of a prototype high-power pulsed laser for adaptive optics. The laser operates at a pulse repetition rate (PRR) of 600–800[Formula: see text]Hz, with a 6% duty cycle. Its coupling efficiency was found to be, in the best test case (using 18[Formula: see text]W of transmitted power), [Formula: see text] photons s[Formula: see text] sr[Formula: see text] atom[Formula: see text] W[Formula: see text] m2 when circular polarization was employed and [Formula: see text] photons s[Formula: see text] sr[Formula: see text] atom[Formula: see text] W[Formula: see text] m2 with linear polarization. No improvement was seen when D[Formula: see text] repumping was used, but this is likely due to the relatively large laser guide star (LGS) diameter, typically 10 arcsec or more, which resulted in low irradiance levels. Strong relaxation oscillations were present in the laser output, which have the effect of reducing the coupling efficiency. To better understand the results, a physical modeling was performed using the measured pulse profiles and parameters specific to these tests. The model results, for a 10 arcsec angular size LGS spot, agree well with the observations. When extrapolating the physical model for a sub-arcsecond angular size LGS (typical of what is needed for a successful astronomical guide star), the model predicts that this laser would have a coupling efficiency of 130 photons s[Formula: see text] sr[Formula: see text] atom[Formula: see text] W[Formula: see text] m2, using circular polarization and D[Formula: see text] repumping, for a LGS diameter of 0.6 arcsec Full Width at Half Maximum (FWHM), and free of relaxation oscillations in the 589 nm laser light.


1993 ◽  
Author(s):  
Peter Hoffmann ◽  
S. Schuberth ◽  
Manfred Geiger ◽  
Claudius Kozlik

1999 ◽  
Vol 27 (2) ◽  
pp. 84-88 ◽  
Author(s):  
Kenichi UEDA

2009 ◽  
Vol 61 (4) ◽  
pp. 763-768
Author(s):  
Meguru Ito ◽  
Yutaka Hayano ◽  
Yoshihiko Saito ◽  
Hideki Takami ◽  
Norihito Saito ◽  
...  

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