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Published byClinton Freeman Modified over 9 years ago
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Broadband Comb-resolved Cavity Enhanced Spectrometer with Graphene Modulator C.-C. Lee, T. R. Schibli Kevin F. Lee C. Mohr, Jie Jiang, Martin E. Fermann Grzegorz Kowzan P. Masłowski
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Spectroscopy cavity enhanced absorption ~ kilometer path length useful for small signals weak transitions low pressures trace concentrations near & mid infrared
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Frequency comb and cavity match comb to resonances graphene in laser cavity modulates loss to control comb offset (CEO)
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Cavity locking compensate for cavity vibrations Pound-Drever-Hall (PDH) locking modulate laser frequency use graphene error signal from reflected light lock laser to cavity
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Schematic
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Modulation graphene modulation of few MHz no external modulator needed reduce etaloning less optical loss lower cost
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Spectrum bandwidth limited by dispersion resonance spacing is chirped LaserCavity transmission
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CO 2 cell filled with air ~400 ppm CO 2 fit to finesse 3600 effective path length of 0.87 km 38 cm long cell one pass would absorb ~0.2% in 30 s, at 0.036 cm -1 resolution SNR ~100 α min = 2×10 -7 cm -1 Fit Data
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Comb-resolved FTIR comb has stable repetition rate and offset measure each comb line match FTIR frequency axis to comb
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Midinfrared OPO 3-6 µm graphene modulation propagates through OPO have locked OPO to cavity at ~3.3 µm
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Summary graphene modulator stabilizes CEO modulates for PDH cavity enhanced spectra high sensitivity high frequency accuracy
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