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Waveguide structures in anisotropic nonlinear crystals

机译:各向异性非线性晶体中的波导结构

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We report on the design and manufacturing parameters of waveguiding structures of anisotropic nonlinear crystals that are employed for harmonic conversions, using Adhesive-Free Bonding (AFB®). This technology enables a full range of predetermined refractive index differences that are essential for the design of single mode or low-mode propagation with high efficiency in anisotropic nonlinear crystals which in turn results in compact frequency conversion systems. Examples of nonlinear optical waveguides include periodically bonded walk-off corrected nonlinear optical waveguides and periodically poled waveguide components, such as lithium triborate (LBO), beta barium borate (p-BBO), lithium niobate (LN), potassium titanyl phosphate (KTP), zinc germanium phosphide (ZGP) and silver selenogallate (AGSE). Simulation of planar LN waveguide shows that when the electric field vector E lies in the k-c plane, the power flow is directed precisely along the propagation direction, demonstrating waveguiding effect in the planar waveguide. Employment of anisotropic nonlinear optical waveguides, for example in combination with AFB® crystalline fiber waveguides (CFW), provides access to the design of a number of novel high power and high efficiency light sources spanning the range of wavelengths from deep ultraviolet (as short as ~200 nm) to mid-infrared (as long as about 18 μm). To our knowledge, the technique is the only generally applicable one because most often there are no compatible cladding crystals available to nonlinear optical cores, especially not with an engineer-able refractive index difference and large mode area.
机译:我们报告了使用无粘合剂键合(AFB®)进行谐波转换的各向异性非线性晶体的波导结构的设计和制造参数。该技术可以实现预定范围的预定折射率差异,这对于各向异性非线性晶体中高效设计单模或低模传播必不可少,从而又可以实现紧凑的频率转换系统。非线性光波导的示例包括定期粘结的走离校正非线性光波导和周期性极化的波导组件,例如三硼酸锂(LBO),β硼酸钡(p-BBO),铌酸锂(LN),钛氧基磷酸钾(KTP) ,磷化锌锗(ZGP)和硒化镓银(AGSE)。平面LN波导的仿真表明,当电场矢量E位于k-c平面时,功率流精确地沿传播方向定向,证明了平面波导中的波导效应。使用各向异性的非线性光波导,例如与AFB®晶体光纤波导(CFW)结合使用,可以设计出许多新颖的高功率和高效光源,其光源范围从深紫外到短波长(短至〜200 nm)到中红外(长达约18μm)。据我们所知,该技术是唯一可普遍应用的技术,因为大多数情况下,非线性光学纤芯没有兼容的包层晶体,特别是没有可设计的折射率差和较大的模面积。

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