用薄LiNbO3夹层结构的金属衬底控制太赫兹产生

S. Bodrov, I. Ilyakov, B. Shishkin, A. Stepanov
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引用次数: 0

摘要

飞秒激光脉冲在电光晶体中传播,通过光整流产生宽带太赫兹辐射。在具有高光学非线性和宽带隙(小多光子吸收)的晶体中,如LiNbO3或LiTaO3,光学群速度比太赫兹波的最高相速度大两倍以上。为了在这种(超光速)晶体中实现相位匹配,可以利用切伦科夫辐射的机制。该方法的主要缺点是典型的强太赫兹吸收(LiNbO3为~ 20 cm−1)和激光泵浦的衍射。为了避免这些限制,有人提出使用薄LiNbO3芯(产生太赫兹辐射并引导激光束)和Si包层(输出低吸收的太赫兹辐射)的平面夹层结构[1]。该方案在实验中显示了目前可用的最高效率(~ 0.1%)[2]。在该方案的进一步发展中,有人提出使用金属衬底将太赫兹发射收集到一个方向,并通过改变金属衬底和LiNbO3层之间的气隙来控制其频谱[3]。在本报告中,我们对该方案进行了实验探索。
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Terahertz generation control by metal substrate in sandwich structure with thin LiNbO3
Femtosecond laser pulses propagating in electro-optic crystal can generate wideband terahertz (THz) radiation via optical rectification. In the crystals with high optical nonlinearities and wide band gaps (small multiphoton absorption), such as LiNbO3 or LiTaO3, the optical group velocity is more than two times larger than the highest phase velocity of terahertz waves. To achieve phase-matching in such (superluminal) crystals the mechanism of Cherenkov radiation may be used. The main drawbacks of this method are typically strong terahertz absorption (∼ 20 cm−1 for LiNbO3) and diffraction of laser pump. To avoid these limitations it was proposed to use a planar sandwich structure with thin LiNbO3 core (to generate THz radiation and guide laser beam) and Si cladding (to output THz radiation with low absorption) [1]. This scheme showed experimentally the highest efficiency available today (∼ 0.1%) [2]. In further development of the scheme it was proposed to use a metal substrate to collect the terahertz emission into one direction and to control its spectrum by varying an air gap between the metal substrate and the LiNbO3 layer [3]. In this presentation we explore this scheme experimentally.
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