Techniques of non-collinear electro-optic sampling for efficient detection of pulsed terahertz radiation

M. Tani, T. Kinoshita, T. Nagase, S. Ozawa, S. Tsuzuki, D. Takeshima, E. Estacio, K. Kurihara, K. Yamamoto, M. Bakunov
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引用次数: 1

Abstract

Cherenkov radiation mechanism is an established technique to achieve phase matching between ultrashort optical pulses and terahertz (THz) waves having a large collinear velocity mismatch, in a nonlinear optical material such as LiNbO3 (LN). Phase matching is achieved with the optical and THz pulses propagating at angle with respect to each other. Recently, we have experimentally demonstrated that Cherenkov phase matching mechanism can also be used for efficient electro-optics (EO) sampling of broadband THz pulses [1]. In the detection case, the phase matching is achieved between an optical and THz pulse propagating non-collinearly at the Cherenkov phase-matching angle θC, satisfying the following equation: equation Here, ngLN is the group index of the EO crystal at the sampling optical wavelength and nTHzLN is the refractive index of the EO crystal in the THz frequency region. An advantage of the non-collinear Cherenkov phase matching is that we can find a corresponding Cherenkov phase matching angle, θC, for any electro-optic crystal at a given optical sampling wavelength. When the EO crystal has a much larger refractive index in THz frequency region compared to that in optical region, a coupling prism is used as illustrated in Fig. 1. Moreover, using a low-loss coupling prism can also reduce absorption in the EO crystal. Silicon is an ideal coupling prism material owing to low absorption losses and is non-dispersive in the THz frequency region. From Snell's law, the incident angle α of THz wave with respect to the prism- EO crystal interface is given as follows: equation Equation (2) leads to the relation, sin β = cosθC. Therefore, Eq. (1) reduces to the following equation for the apex angle of the coupling prism (α) at the Cherenkov phase-matching condition given by the ratio of the group index of the EO crystal at the sampling optical wavelength ngLN, and the refractive index of Si, nTHzSi, in the THz frequency region: equation.
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用于脉冲太赫兹辐射有效检测的非共线电光采样技术
切伦科夫辐射机制是一种在非线性光学材料(如LiNbO3 (LN))中实现超短光脉冲与具有较大共线速度失配的太赫兹(THz)波之间相位匹配的成熟技术。相位匹配是通过光脉冲和太赫兹脉冲以相对于彼此的角度传播来实现的。最近,我们通过实验证明,切伦科夫相位匹配机制也可以用于宽带太赫兹脉冲的高效电光(EO)采样[1]。在检测情况下,光脉冲与太赫兹脉冲以切伦科夫相位匹配角θC非共线传播,实现相位匹配,满足如下式:式中,ngLN为采样光波长处EO晶体的群折射率,nTHzLN为太赫兹频率区域EO晶体的折射率。非共线切伦科夫相位匹配的一个优点是,在给定的光学采样波长下,我们可以找到任何电光晶体对应的切伦科夫相位匹配角θC。当EO晶体在太赫兹频率区的折射率远大于光区折射率时,采用如图1所示的耦合棱镜。此外,使用低损耗耦合棱镜也可以减少EO晶体的吸收。硅具有吸收损耗低、在太赫兹频段内无色散等特点,是理想的耦合棱镜材料。由斯涅尔定律可得太赫兹波相对于棱镜- EO晶体界面的入射角α:式(2)可得sin β = cosθC的关系式。因此,在切伦科夫相位匹配条件下,由EO晶体在采样光波长ngLN处的群折射率与Si在太赫兹频率区域的折射率nTHzSi之比给出的耦合棱镜顶点角(α),式(1)简化为:
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