Author Affiliations
1Key Laboratory of Atmospheric Optics, Anhui Institute of Optics and Fine Mechanics, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, Anhui, China2Science Island Branch, Graduate School, University of Science and Technology of China, Hefei 230026, Anhui, China3Advanced Laser Technology Laboratory of Anhui Province, Hefei 230037, Anhui, China4A Department in Mianyang, Space System Department, Mianyang 621000, Sichuan, Chinashow less
Fig. 1. Simulation diagram of V-shaped cavity
Fig. 2. Spot distributions on M1 and M2 surfaces at different angles
Fig. 3. Spot distributions on lens M2 surface at different off-axis incidence angles
Fig. 4. Intensity distributions of light emitting from surface of cavity mirror for V-OA-ICOS and OA-ICOS. (a) V-OA-ICOS; (b) OA-ICOS
Fig. 5. Structure design of V-shaped cavity
Fig. 6. V-OA-ICOS experimental measuring device
Fig. 7. Cavity mode signals at different off-axis incidence angles.(a) γ1; (b) γ2; (c) γ3
Fig. 8. Measurement data of V-OA-ICOS device. (a) CO2 absorption spectrum; (b) residual of Voigt fitting
Fig. 9. Measurement results of standard CO2 gas with volume fraction of 400×10-6 during 50 min. (a) Stability test; (b) Allan variance
Fig. 10. Simulated absorption spectra of CO2, H2O, and NH3 near 4987 cm-1
Fig. 11. NH3 absorption spectrum and Savitzky-Golay smoothing results at different window widths. (a) Raw absorption spectrum; spectral data obtained after smoothing by Savitzky-Golay algorithm when window width is (b) 30, (c) 40, (d) 50, (e) 60, and (f) 70
Fig. 12. NH3 absorption spectrum and Voigt fitting residual of V-OA-ICOS device. (a) Before smoothing by Savitzky-Golay algorithm; (b) after smoothing by Savitzky-Golay algorithm