首页> 外文期刊>Applied Physics Letters >Widely tunable and monochromatic terahertz difference frequency generation with organic crystal 2-(3-(4-hydroxystyryl)-5, 5-dime-thylcyclohex-2-enylidene)malononitrile
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Widely tunable and monochromatic terahertz difference frequency generation with organic crystal 2-(3-(4-hydroxystyryl)-5, 5-dime-thylcyclohex-2-enylidene)malononitrile

机译:有机晶体2-(3-(4-羟基苯乙烯基)-5,5-dime-thylcyclohex-2-enylidene)丙二腈的可广泛调谐和单色太赫兹差分频率产生

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摘要

We report an experimental study on widely tunable terahertz (THz) wave difference frequency generation (DFG) with hydrogen-bonded crystals 2-(3-(4-hydroxystyryl)-5,5-dime-thylcyclohex-2-enylidene) malononitrile (OH1). The organic crystals were pumped by a ~1.3μm double-pass KTiOPO_4 optical parametric oscillator. A tuning range of 0.02-20 THz was achieved. OH1 crystals offer a long effective interaction length (also high output) for the generation below 3 THz, owing to the low absorption and favorable phase-matching. The highest energy of 507 nJ/pulse was generated at 1.92 THz with a 1.89-mm-thick crystal. Comprehensive explanations were provided, on the basis of theoretical calculations. Cascading phenomenon during the DFG process was demonstrated. The photon conversion efficiency could reach 2.9%.
机译:我们报告了与氢键合晶体2-(3-(4-羟基苯乙烯)-5,5-二甲基-乙基环己-2-烯基)丙二腈(OH1)的可广泛调谐的太赫兹(THz)波差频率产生(DFG)的实验研究)。有机晶体由〜1.3μm双通道KTiOPO_4光学参量振荡器泵浦。实现了0.02-20 THz的调谐范围。 OH1晶体由于其低吸收和良好的相位匹配,可为3 THz以下的晶体提供长的有效相互作用长度(也具有高输出)。在1.92 THz的频率下,厚度为1.89 mm的晶体产生的最高能量为507 nJ /脉冲。在理论计算的基础上提供了全面的解释。演示了DFG过程中的级联现象。光子转换效率可以达到2.9%。

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  • 来源
    《Applied Physics Letters》 |2016年第1期|011104.1-011104.3|共3页
  • 作者单位

    The Institute of Laser and Optoelectronics, College of Precision Instruments and Opto-electronics Engineering, Tianjin University, Tianjin 300072, China,The Key Laboratory of Weak-Light Nonlinear Photonics, Ministry of Education, School of Physics and TEDA Applied Physics Institute, Nankai University, Tianjin 300071, China;

    Beijing Center for Crystal Research and Development, Key Laboratory of Functional Crystals and Laser Technology, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China,University of Chinese Academy of Sciences, Beijing 100049, China;

    The Institute of Laser and Optoelectronics, College of Precision Instruments and Opto-electronics Engineering, Tianjin University, Tianjin 300072, China;

    The Institute of Laser and Optoelectronics, College of Precision Instruments and Opto-electronics Engineering, Tianjin University, Tianjin 300072, China;

    Beijing Center for Crystal Research and Development, Key Laboratory of Functional Crystals and Laser Technology, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China;

    The Institute of Laser and Optoelectronics, College of Precision Instruments and Opto-electronics Engineering, Tianjin University, Tianjin 300072, China;

    Beijing Center for Crystal Research and Development, Key Laboratory of Functional Crystals and Laser Technology, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China;

    The Key Laboratory of Weak-Light Nonlinear Photonics, Ministry of Education, School of Physics and TEDA Applied Physics Institute, Nankai University, Tianjin 300071, China;

    The Institute of Laser and Optoelectronics, College of Precision Instruments and Opto-electronics Engineering, Tianjin University, Tianjin 300072, China;

    Beijing Center for Crystal Research and Development, Key Laboratory of Functional Crystals and Laser Technology, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China;

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