Comparison of semiclassical line-shape models to rovibrational spectra measured by frequency-stabilized cavity ring-down spectroscopy
A single-mode cavity ring-down spectrometer, which incorporates a stabilized and tuneable
comb of resonant frequencies and a continuous-wave external-cavity diode probe laser, was
used to study rovibrational absorption line shapes within the 2 ν 1+ ν 3 and 3 ν 3 vibrational
bands of water vapor. This spectrometer, which has a noise-equivalent absorption
coefficient of 2× 10− 9 cm− 1 Hz− 1∕ 2 and frequency resolution of 50 kHz, enables high-
precision measurements of line-shape effects and pressure shifting of relatively weak …
comb of resonant frequencies and a continuous-wave external-cavity diode probe laser, was
used to study rovibrational absorption line shapes within the 2 ν 1+ ν 3 and 3 ν 3 vibrational
bands of water vapor. This spectrometer, which has a noise-equivalent absorption
coefficient of 2× 10− 9 cm− 1 Hz− 1∕ 2 and frequency resolution of 50 kHz, enables high-
precision measurements of line-shape effects and pressure shifting of relatively weak …
A single-mode cavity ring-down spectrometer, which incorporates a stabilized and tuneable comb of resonant frequencies and a continuous-wave external-cavity diode probe laser, was used to study rovibrational absorption line shapes within the and vibrational bands of water vapor. This spectrometer, which has a noise-equivalent absorption coefficient of and frequency resolution of , enables high-precision measurements of line-shape effects and pressure shifting of relatively weak absorption transitions. We investigated the room-temperature pressure dependence over the range from of two transitions perturbed by He, , and . Foreign-gas broadening and pressure-shift coefficients were determined for a relatively strong transition at , and for a weaker transition at the self- and -broadening and pressure-shift parameters were measured. In the low-pressure limit the room-temperature Doppler width was measured within 0.2% of its expected value. Doppler-free saturation effects were also observed with linewidths below . The data were compared to semiclassical line-shape models that considered the influence of Dicke narrowing as well as the speed dependence of pressure broadening and pressure shifting. Taking both of these effects into account gave the best agreement with our observations and allowed us to model the observed asymmetries of experimental profiles. Hard- and soft-collision as well as billiard-ball collision models were considered. These results allowed us to quantify systematic errors in line intensity and in pressure broadening associated with oversimplified models of line shape.
American Physical Society
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