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A Theoretical Study on Special Ti:LiNbO Structure of an Array of Strip Waveguides Embedded in a Planar Waveguide

机译:嵌入平面波导中的条形波导阵列的特殊Ti:LiNbO结构的理论研究

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A theoretical study was performed on waveguiding characteristics of a special Ti:LiNbO$_{3}$ structure that an array of strip waveguides is embedded in a planar waveguide. First, a special Ti:LiNbO$_{3}$ structure was fabricated by diffusion of homogeneously coated Ti film at first and then photolithographically patterned Ti-strips with different widths of 4, 5, 6, 7, and 8 $mu$ m, and the transverse magnetic (TM) mode guided in the strip waveguides of the special structure was characterized by near-field measurements. Second, a 2-D refractive index profile is supposed for the special structure. Third, based upon this supposed index profile model and the experimentally determined mode field profile type, the mode sizes of the strip waveguides were calculated using variational method and compared with the experimental results to verify the validity of the index model supposed and the numerical method adopted. Finally, the mode sizes and effective indexes of several lowest order TM modes guided in the strip waveguides were calculated as a function of the initial Ti-strip width for different waveguide parameters that include the surface index increment and depth (width) of both the planar and strip waveguides. The numerical results show that the field profile in the width direction is influenced by many factors such as the initial Ti-strip width, waveguide width and depth, and the surface index increment of the strip waveguide. Instead, the mode field in the depth direction is only influenced by three factors that include the depth of strip waveguide and the surface index increments of both planar and strip waveguides. The single-mode condition depends on all of these parameters.
机译:对特殊的Ti:LiNbO $ _ {3} $结构的波导特性进行了理论研究,该结构将条形波导阵列嵌入平面波导中。首先,首先通过扩散均匀涂覆的Ti膜,然后通过光刻图案化具有4、5、6、7和8 $μm的不同宽度的Ti条,来制造特殊的Ti:LiNbO $ _ {3} $结构。 ,并通过近场测量来表征在特殊结构的条形波导中引导的横向磁(TM)模式。其次,对于特殊结构,应假定二维折射率分布。第三,基于该假设的折射率分布模型和实验确定的模场分布类型,使用变分法计算带状波导的模大小,并与实验结果进行比较,以验证假设的折射率模型和采用的数值方法的有效性。 。最后,针对不同的波导参数(包括平面的表面折射率增量和深度(宽度)),计算在条形波导中导引的几种最低阶TM模的模大小和有效折射率,作为初始Ti条纹宽度的函数和条形波导。数值结果表明,宽度方向上的场分布受到许多因素的影响,例如初始Ti条纹宽度,波导宽度和深度以及带状波导的表面折射率增量。取而代之的是,深度方向上的模场仅受三个因素的影响,包括带状波导的深度以及平面和带状波导的表面折射率增量。单模条件取决于所有这些参数。

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