Chinese Physics B, Volume. 29, Issue 10, (2020)
Dependence of interferogram phase on incident wavenumber and phase stability of Doppler asymmetric spatial heterodyne spectroscopy
Fig. 1. (a) Schematic diagram of typical DASH interferometer, where L1 and L2 are collimating lenses. L3 and L4 are imaging lenses, gratings 1 and 2 are tilted by a Littrow angle
Fig. 2. Schematic diagram of wavefronts movement approximation, where red and blue lines represent wavefronts and arrows denote the direction of approximated wavefronts.
Fig. 3. FOV effects and comparisons at [(a) and (c)] 15873 cm−1 and [(b) and (d)] 15803 cm−1. Red lines represent results calculated from Eq. (
Fig. 4. Phase comparisons of OPD offset effect (a) at 15873 cm−1 and (b) at 15803 cm−1. Red lines represent results calculatedfrom Eq. (
Fig. 5. (a) Averaged interferogram from five recorded pictures. (b) Analysis signal generated from the selected area shown in panel (a). (c) Schematic diagram of inversion phase from analysis signal shown in panel (b). Blue points indicate the retrieved raw phase and red points reptrsent the unwrapped phase.
Fig. 6. Phase variations at 512nd pixel when grating on the linear stage is gradually moved.
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Ya-Fei Zhang, Yu-Tao Feng, Di Fu, Peng-Chong Wang, Jian Sun, Qing-Lan Bai. Dependence of interferogram phase on incident wavenumber and phase stability of Doppler asymmetric spatial heterodyne spectroscopy[J]. Chinese Physics B, 2020, 29(10):
Received: Jan. 7, 2020
Accepted: --
Published Online: Apr. 21, 2021
The Author Email: Yu-Tao Feng (fytciom@126.com)