研究目的
To demonstrate frequency-domain differential absorption spectroscopy in the terahertz (THz) frequency region using spectral multifurcated oscillations in a passively Q-switched microchip laser.
研究成果
The study successfully demonstrated THz-wave differential absorption spectroscopy using a multifurcated subnanosecond microchip laser. The technique eliminates the need for active frequency modulation, offering simple and robust operation for real-time monitoring of gas molecules. The system's flexibility allows for monitoring of various gas molecules by tuning THz-wave frequencies within the is-TPG tuning range. This approach opens new pathways for the realization of THz differential absorption lidars for fast gas sensing applications.
研究不足
The current laser repetition rate is equal to the AC electric frequency of 50 Hz in eastern Japan, which may limit the measurement rate. The frequency linewidth of the order of 5 GHz, while suitable for spectroscopic detection, may not be sufficient for all applications requiring higher resolution.
1:Experimental Design and Method Selection:
The study utilized a passively Q-switched microchip laser to generate multifurcated subnanosecond pulses for THz-wave differential absorption spectroscopy. The laser was end-pumped by a fiber-coupled high-power 808-nm vertical-cavity surface-emitting laser (VCSEL) module.
2:Sample Selection and Data Sources:
The system was tested with water vapor in atmospheric air as the sample.
3:List of Experimental Equipment and Materials:
A microchip laser comprising a 7-mm-long Nd:YAG/Cr:YAG composite ceramic, a VCSEL module, an external cavity diode laser (ECDL), an Yb-doped fiber amplifier (YDFA), a MgO-doped LiNbO3 crystal for THz-wave parametric generation, and a Schottky-barrier-diode (SBD) receiver.
4:Experimental Procedures and Operational Workflow:
The microchip laser was operated under QCW end-pumping to generate multifurcated pulses. These pulses were used to drive an injection-seeded THz-wave parametric generator. The THz-wave output was detected using an SBD receiver after passing through a gas cell.
5:Data Analysis Methods:
The output signal from the SBD receiver was analyzed using an analog-to-digital converter (ADC) with a sampling rate of 100 MS/s.
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