LSC meeting, Hanford, 2002 LIGO-G020377-00-Z Remote in situ monitoring of weak distortions Ilya Kozhevatov, Efim Khazanov, Anatoly Poteomkin, Anatoly Mal’shakov,

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Presentation transcript:

LSC meeting, Hanford, 2002 LIGO-G Z Remote in situ monitoring of weak distortions Ilya Kozhevatov, Efim Khazanov, Anatoly Poteomkin, Anatoly Mal’shakov, Nikolay Andreev, Andrey Shaykin, Alexander Sergeev Remote in situ monitoring of weak distortions Ilya Kozhevatov, Efim Khazanov, Anatoly Poteomkin, Anatoly Mal’shakov, Nikolay Andreev, Andrey Shaykin, Alexander Sergeev Institute of Applied Physics of the Russian Academy of Sciences, , Nizhny Novgorod, Russia

Current Research  Remote in situ monitoring of weak distortions emerging under auxiliary laser heating similarly to what is expected in advanced LIGO core optics  Proposal for remote in situ monitoring of weak distortions of ETM.

Remote in situ monitoring of weak distortions emerging under auxiliary laser heating  Optical sample bulk heating by the fundamental or second harmonic of Nd:YAG laser at a power of W  Surface heating with the use of a CO 2 laser at power of several Watts  Inducing contamination of a small region (characteristic size of micron) on the optical element's surface and focusing of low-power laser radiation (<100 mW) on it 2 Vacuum chamber Heating CO 2 laser Sample Heating Nd laser 1 - WLPMI 2 - NHS and PIT

Scanning Linear HartmannTechnique F Rotating mirror CW diode laser Sample CCD camera F F  1d scan over 50 mm requires 60 s (120 data points), mainly due to computer processing (maximum extracting)  25 Hz standard video output CCD camera  1064 nm CW single-mode laser diode with few milliwatt in fiber output  1d scan over 50 mm requires 60 s (120 data points), mainly due to computer processing (maximum extracting)  25 Hz standard video output CCD camera  1064 nm CW single-mode laser diode with few milliwatt in fiber output PC

Optical depth profile measured with scanning linear Hartmann sensor for two heating beam : 7mm Airy and 1 mm pencil structures

White Light In Situ Measurement Interferometer (WLISMI) White Light In Situ Measurement Interferometer (WLISMI)

White Light In Situ Measurement Interferometer. Experimental setup White Light In Situ Measurement Interferometer. Experimental setup 1 - light source; 2 - objective; 3 - sample; 4 - ocular; 5 - measurement interferometer; 6 - unit for synchroni- zation and control; 7 - CCD camera; 8 - PC computer; 9 - modulating mirror; 10 - adjusting mirror; 11, 13 - motors; 12 - wave front shaper

White Light In Situ Measurement Interferometer Phase Map White Light In Situ Measurement Interferometer Phase Map

 Phase map of optical sample heated by CO 2 laser Thickness - 15 mm Diameter - 85 mm Place of heating beam

Simultaneous measurements of optical depth profiles under heating using two different techniques СO 2 laser mW Beam size - 7 mm Simultaneous measurements of optical depth profiles under heating using two different techniques СO 2 laser mW Beam size - 7 mm WLISMI Hartmann

White Light In Situ Measurement Interferometer. How to install in LIGO interferometer? White Light In Situ Measurement Interferometer. How to install in LIGO interferometer?

White Light In Situ Measurement Interferometer. How to install in LIGO interferometer? White Light In Situ Measurement Interferometer. How to install in LIGO interferometer?

Experimental results. No heating. rms=0.32nm ( /2000)

Experimental results. Heated by CO 2 laser.

Conclusion  LIGO-IAP Lab has been equipped with several instruments developed at IAP for High-Precision Characterization of LIGO Optical Components  25 cm aperture white-light phase-modulated interferometer (WLPMI) for preliminary control of LIGO Core Optics has been implemented  Simultaneous measurements of optical depth profiles under heating using two different techniques have been performed  Version of WLPMI for installation on end station is tested experimentally.