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High-energy and ultra-wideband tunable monochromatic terahertz source and frequency domain spectroscopy system based on DAST crystal

机译:基于DAST晶体的高能超宽带可调谐单色太赫兹源和频域光谱系统

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摘要

We have demonstrated a high-energy and broadly tunable monochromatic terahertz (THz) source via differencefrequency generation (DFG) in DAST crystal. The THz frequency is tuned randomly in the range of 0.3-19.6 THz, whichis much wider than the THz source based on the inorganic crystal and the photoconductive antenna. The highest energyof 2.53μJ/pulse is obtained at 18.9 THz corresponding to the optical-to-optical conversion efficiency of 1.31×10~(-4). TheTHz output spectroscopy is theoretically and experimentally explained by DFG process and Raman spectroscopy.Meanwhile, a phenomenon of blue light from the KTP-OPO with tunable and multiple wavelengths was firstly observedand explained. Based on our THz source, an ultra-wideband THz frequency domain system (THz-FDS) withtransmission mode is realized to measure the ultra-wideband THz spectroscopies of typical materials in solid and liquidstates, such as Si, SiC, White PE, water, isopropyl myristate, simethicone, atonlein and oleic acid, etc.. Furthermore, wehave studied the THz spectral characteristic of biomedical tissue in the ultra-wideband THz frequency range of 0.3-15THz to study the biomedical response in the entire THz frequency range, which contains more abundant spectralinformation and was rarely focused with the limit of the THz source.
机译:我们已经通过DAST晶体中的差\ r \ n频率产生(DFG)展示了一种高能量且可广泛调谐的单色太赫兹(THz)源。太赫兹频率在0.3-19.6太赫兹范围内随机调谐,比基于无机晶体和光电导天线的太赫兹源宽得多。在18.9 THz处获得最高能量\ r \ n为2.53μJ/脉冲,对应的光光转换效率为1.31×10〜(-4)。通过DFG工艺和拉曼光谱在理论上和实验上解释了\ r \ nTHz输出光谱。\ r \ n同时,首先解释了来自KTP-OPO的蓝光现象具有可调谐和多种波长。基于我们的太赫兹源,实现了具有\ r \ n传输模式的超宽带太赫兹频域系统(THz-FDS),用于测量固态和液态\ r \ n状态下典型材料的超宽带太赫兹光谱,SiC,白色PE,水,肉豆蔻酸异丙酯,二甲硅油,牛油蛋白和油酸等。此外,我们已经研究了生物医学组织在0.3-r超宽带THz频率范围内的THz光谱特性。 n15THz用于研究整个THz频率范围内的生物医学响应,该频谱包含更丰富的频谱信息,很少关注THz源的限制。

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    Institute of Laser and Optoelectronics, School of Precision Instrument and Opto-electronics Engineering, Tianjin University, Tianjin 300072, People’s Republic of China Key Laboratory of Opto-electronics Information Technology (Tianjin University), Ministry of Education, Tianjin 300072, People’s Republic of China;

    Institute of Laser and Optoelectronics, School of Precision Instrument and Opto-electronics Engineering, Tianjin University, Tianjin 300072, People’s Republic of China Key Laboratory of Opto-electronics Information Technology (Tianjin University), Ministry of Education, Tianjin 300072, People’s Republic of China yuyewang@tju.edu.cn;

    Institute of Laser and Optoelectronics, School of Precision Instrument and Opto-electronics Engineering, Tianjin University, Tianjin 300072, People’s Republic of China Key Laboratory of Opto-electronics Information Technology (Tianjin University), Ministry of Education, Tianjin 300072, People’s Republic of China;

    Institute of Laser and Optoelectronics, School of Precision Instrument and Opto-electronics Engineering, Tianjin University, Tianjin 300072, People’s Republic of China Key Laboratory of Opto-electronics Information Technology (Tianjin University), Ministry of Education, Tianjin 300072, People’s Republic of China;

    Institute of Laser and Optoelectronics, School of Precision Instrument and Opto-electronics Engineering, Tianjin University, Tianjin 300072, People’s Republic of China Key Laboratory of Opto-electronics Information Technology (Tianjin University), Ministry of Education, Tianjin 300072, People’s Republic of China;

    Institute of Laser and Optoelectronics, School of Precision Instrument and Opto-electronics Engineering, Tianjin University, Tianjin 300072, People’s Republic of China Key Laboratory of Opto-electronics Information Technology (Tianjin University), Ministry of Education, Tianjin 300072, People’s Republic of China;

    Institute of Laser and Optoelectronics, School of Precision Instrument and Opto-electronics Engineering, Tianjin University, Tianjin 300072, People’s Republic of China Key Laboratory of Opto-electronics Information Technology (Tianjin University), Ministry of Education, Tianjin 300072, People’s Republic of China;

    Institute of Laser and Optoelectronics, School of Precision Instrument and Opto-electronics Engineering, Tianjin University, Tianjin 300072, People’s Republic of China Key Laboratory of Opto-electronics Information Technology (Tianjin University), Ministry of Education, Tianjin 300072, People’s Republic of China;

    College of Physics, Qingdao University, Qingdao 266071, People’s Republic of China Key Laboratory of Photonics Materials and Technology in Universities of Shandong (QingdaoUniversity), Qingdao 266071, People’s Republic of China;

    Institute of Laser and Optoelectronics, School of Precision Instrument and Opto-electronics Engineering, Tianjin University, Tianjin 300072, People’s Republic of China Key Laboratory of Opto-electronics Information Technology (Tianjin University), Ministry of Education, Tianjin 300072, People’s Republic of China;

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