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Brian Siller, Andrew Mills & Benjamin McCall University of Illinois at Urbana-Champaign
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Positive column discharge cell ◦ High ion density, rich chemistry ◦ Cations move toward the cathode Plasma Discharge Cell +1kV-1kV
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Positive column discharge cell ◦ High ion density, rich chemistry ◦ Cations move toward the cathode ◦ Ions absorption profile is Doppler-shifted Plasma Discharge Cell +1kV-1kV Laser Detector
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Positive column discharge cell ◦ High ion density, rich chemistry ◦ Cations move toward the cathode ◦ Ions absorption profile is Doppler-shifted Plasma Discharge Cell -1kV+1kV Laser Detector
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Positive column discharge cell ◦ High ion density, rich chemistry ◦ Cations move toward the cathode ◦ Ions absorption profile is Doppler-shifted Drive with AC voltage ◦ Ion Doppler profile alternates red/blue shift ◦ Laser at fixed wavelength ◦ Demodulate detector signal at modulation frequency Plasma Discharge Cell Detector Laser
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Want strongest absorption possible Signal enhanced by modified White cell ◦ Laser passes through cell unidirectionally ◦ Can get up to ~8 passes through cell Plasma Discharge Cell Laser Detector
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Optical cavity acts as a multipass cell ◦ Number of passes = ◦ For finesse of 150, get ~100 passes Must actively lock laser wavelength/cavity length to be in resonance with one another DC signal on detector is extremely noisy ◦ Velocity modulation with lock-in amplifier minimizes effect of noise on signal detection Laser Cavity Detector
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Cavity Transmission Error Signal Ti:Sapph Laser EOM PZT Lock Box 14MHz Detector
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Lock-In Amplifier Transformer Cavity Mirror Mounts Audio Amplifier Laser 40 kHz
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Doppler profile shifts back and forth Red-shift with respect to one direction of the laser corresponds to blue shift with respect to the other direction Net absorption is the sum of the absorption in each direction Absorption Strength (Arb. Units) Relative Frequency (GHz)
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V (kV) t (μs) Absorption Relative Frequency
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Demodulate detected signal at twice the modulation frequency (2f) Can observe and distinguish ions and neutrals ◦ Ions are velocity modulated ◦ Excited neutrals are concentration modulated ◦ Ground state neutrals are not modulated at all
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Cavity Finesse 150 30mW laser power N 2 + Meinel Band N 2 * first positive band Second time a Lamb dip of a molecular ion has been observed (first was DBr + in laser magnetic resonance technique) 1 Used 2 lock-in amplifiers for N 2 + /N 2 * 1 M. Havenith, M. Schneider, W. Bohle, and W. Urban; Mol. Phys. 72, 1149 (1991).
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N2+N2+ ◦ Velocity directly dependent on voltage ◦ No significant phase shift with respect to voltage N2*N2* ◦ 78° phase shift with respect to N 2 + signal ◦ Peak N 2 * density occurs when rate of formation equals rate of destruction V (kV) t (μs) Peak N 2 * Density
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N 2 + ◦ Velocity directly dependent on voltage ◦ No significant phase shift with respect to voltage N 2 * ◦ 78° phase shift with respect to N 2 + signal ◦ Peak N 2 * density occurs when rate of formation equals rate of destruction ◦ Analogous to Earth’s heating/cooling cycle with the sun Sun is brightest at noon (peak voltage) Hottest time of day is 5pm (peak N 2 * density) 5 hour time delay in 24 hour day = 75° phase shift
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Potentially orders of magnitude more sensitivity Allows for saturation spectroscopy ◦ Resolve Doppler-blended lines ◦ Better line center determination ◦ Width of Lamb dip allows more information to be extracted from spectra (See talk FD02 for much more detail)
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Better isolation of plasma noise ◦ Faraday cage ◦ Dedicated grounding Improved cavity locking ◦ Less noise induced by lock to cavity ◦ Allow for locking to a higher finesse cavity Heterodyne Detection
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Improves upon absorption strength of velocity modulation experiments Allows for Doppler-free spectroscopic studies of molecular ions Very general technique To unlock full potential, must first minimize plasma noise with careful experimental setup
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McCall Group Funding ◦ Air Force ◦ NASA ◦ Dreyfus ◦ Packard ◦ NSF ◦ Sloan
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