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Fig. 2.

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FTMW hyperfine spectrum of 31, 2 − 30, 3 rotational transition for NCCHCS. Each hyperfine component is split into two Doppler components because the direction of the supersonic jet expansion is parallel to the standing wave in the Fabry-Pérot cavity of the spectrometer. The spectra were achieved by 300 shots of accumulation and a step scan of 1.0 MHz with a repetition rate of 10 Hz.

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