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Novel detection of aerosols: combined cavity ring-down and fluorescence spectroscopy

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Abstract

High fluences inside cavity ring-down spectroscopy optical resonators lend themselves to fluorescence or nonlinear optical spectroscopy. An instrument at 488 nm was developed to measure extinction, and fluorescence of aerosols. A detection limit of 6×10-9 cm- 1Hz-1/2 (0.6 Mm-1Hz-1/2) was achieved. The fluorescence spectral power collected from a single fluorescent microsphere was 10 to 20 pW/nm. This power is sufficient to obtain the spectrum of a single microsphere with a resolution of 10 nm and signal-to-noise ratio of ~10. The relative concentrations of two types of fluorescent microspheres were determined from a time-integrated fluorescence measurement of a mixture of both.

©2005 Optical Society of America

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Figures (5)

Fig. 1.
Fig. 1. (Bottom) Cavity ring-down system used for simultaneous measurement of extinction and fluorescence of aerosols. (Top left): photograph of system, (Top right): rendering of the ring-down cavity with fluorescence detection optics attached.
Fig. 2.
Fig. 2. (a) Cutaway view inside ring-down cavity showing the optical path and (b) gas handling system for ring-down system.
Fig. 3.
Fig. 3. Measured ring-down time in air over 1000 events (ring-downs).
Fig. 4.
Fig. 4. Comparison between: (a) 550 nm fluorescence channel and ring-down detector, (b) 650 nm fluorescence channel and ring-down detector, and (c) 550 nm and 650 nm channels.
Fig. 5.
Fig. 5. Correlation between integrated fluorescence signals from the 550 nm and 650 nm fluorescence detectors when using the 550 nm microspheres.

Equations (6)

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I ( t , λ ) = I o e t τ ( λ )
σ ext = 1 c ( 1 τ aer 1 τ 0 )
α min = 1 l eff ( Δ τ τ ) ,
I intracavity = P c T ξ 1 R
Ω = 4 π sin ( θ 4 ) 2
[ 550 spheres 650 spheres ] = [ 0.7 0.024 0.336 2 ] [ 550 channel 650 channel ]
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