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Published byHope Rice Modified over 8 years ago
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Photo-thermal Deflection Spectroscopy George Noid LIGO SURF Student
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Summary Introduction Theory Experiment Results
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LIGO TEST MASSES Fused Silica – Currently uses – Thermal Conductivity is 1.38 W/mK Synthetic Sapphire – Proposed for LIGO II – Crystal Systems – Thermal Conductivity is 23.1 parallel to optical axis
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Photothermal Deflection Spectroscopy (PDS) PDS First used: 1979 Two Lasers: – Pump – Probe Temperature Gradient => Gradient in the index of refraction Useful as a non-destructive spectroscopic method – Can observe microscopic impurities in a crystal – Ex: trace metals in a sapphire crystal
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PDS Probe – Does not disturb sample – Detected Pump - More powerful - Modulated - Not detected
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Deflection
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Deflection (cont.) Snells law: a sin A = b sin B (..) = arcsin { (n 0 )/(n(..)) * sin (pi/2 - )} – = laser angles – = angle of deflection – n 0 = index of refraction of sapphire (1.862) – n = index of refraction function caused by PDS
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The Experiment: two laser tables Pump table – 700 mW Nd YAG laser – Chopper – Fiber coupler – Fiber Probe table – 5 mW He Ne – Fiber – Telescope – 1064 mirror – Biconvex lens – Sapphire crystal – Quad cell Detetector
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Pump Table Nd YAG chopper 5- axis fiber aligner Polarization Selecting filter
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Injecting and Maximizing
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Probe table Photo detector sample He Ne laser Fiber conduit telescope Fiber chuck Aspheric lens holder 1064 mirror beam tube XY stage XYZ stage
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Probe Table: laser alignment Small angle theta in the y direction – Increases interaction length Beam waists: 80 microns Nd Yag – Magnified, collimated in telescope – Reflected off mirror – Focused in biconvex lens into sapphire He - ne – Passes through 1064 mirror – Focused in biconvex lens into sapphire
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Data Initial results were inconclusive with lock- in amplification. Observed PDS with signal analyzer Pump power incident: 300 mw Chopping frequency: 500 Hz Maximum signal to noise ratio: 27 to 3 Crystal mapping ongoing
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Representative Peak
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