Photonics Research, Volume. 10, Issue 2, 340(2022)
Near-optimal intense and powerful terahertz source by optical rectification in lithium niobate crystal
Fig. 1. Experimental setup for the generation and detection of THz pulses with the LN and their detection by EO sampling. BS, beam splitter;
Fig. 2. Measured characteristics of the probe pulse after temporal compression. (a) Spectral amplitude and spectral phase distribution with the image of the probe spot in the inset; (b) temporal intensity and temporal phase distribution.
Fig. 3. Pump spot image. (a) 1 mm before the image plan position; (b) at the image plan position; and (c) 1 mm after the image plan position; (d) horizontal profile of the pump spot at the focus position; (e) normalized pump spectra at the entrance and the exit of the LN crystal after OR process.
Fig. 4. THz beam radius at several locations along its propagation path (a) at the LN crystal exit facet; (b) along the focus of the OAEM; (c) along the focus of the third off-axis mirror, which corresponds to the positions
Fig. 5. (a) Temporal evolution of the generated THz pulse detected by EO sampling in an unpurged environment, with the zoom view of the temporal evolution of the THz pulse in a purged environment in the inset; (b) normalized spectrum of the generated THz pulse in an unpurged environment, with the normalized spectrum at logarithmic scale in the inset.
Fig. 6. Normalized THz transmission through the InGaAs sample as a function of
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L. Guiramand, J. E. Nkeck, X. Ropagnol, T. Ozaki, F. Blanchard, "Near-optimal intense and powerful terahertz source by optical rectification in lithium niobate crystal," Photonics Res. 10, 340 (2022)
Category: Lasers and Laser Optics
Received: Apr. 20, 2021
Accepted: Nov. 21, 2021
Published Online: Jan. 11, 2022
The Author Email: F. Blanchard (francois.blanchard@etsmtl.ca)