导波光学中电光铁电材料的可取性

R. Holman, L.M. Althouse Johnson, D. Skinner
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引用次数: 8

摘要

一个说明性的,器件-系统级的可取性优化分析已经执行了一些重要的电光材料,候选用于高速导波光学器件。研究了高、低温转变材料、立方晶体、有机晶体和合金半导体。采用体导波相位调制器作为初始筛选装置。性能指标,如电力供应限制和设备的最大运行速度,作为系统变量的函数进行了分析,包括材料特性和电极结构。可取性分析已被提出作为一个复合的数学函数,描述了两个或多个独立的性能措施,根据所有相关的系统变量。该函数以图形方式显示,以识别那些共同优化性能度量的系统变量集。最初的筛选分析忽略了传输损耗和电场与光场之间不理想的重叠。铌酸钾、钛酸钡和铌酸锂已被发现是最理想的电光材料。使用几千埃厚度的介电缓冲层是隔离调制器和高介电常数、高强度材料(如钾缓冲层)的必要条件,然而,当使用介电常数和低电光效应材料(如铌酸锂)时,通常是不必要的。电解IC铌酸盐制备的阴极。应该是较低的c强度
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Desirability of Electrooptic Ferroelectric Materials for Guided-Wave Optics
An illustrative, device-systems-level desirability optimization analysis has been performed for a number of important electrooptic materials that are candidate for use in high-speed guided-wave optical devices. Ferroel ect r ic materials with high and low transition temperatures, cubic crystals, organic crystals, and alloy semiconductors have been considered. The bulk guided-wave phase modulator has been taken as the initial screening device. Performance measures such as electrical power supply constraints and the device's maximum operating speed have been analyzed as a function of system variables that include material properties and electrode architectures. Desirability analysis has been presented as a composite mathematical function that describes two or more independent performance measures in terms of all relevant system variables. This function has been displayed graphically to identify those sets of system variables that jointly optimize the performance measures o f greatest interest. The initial screening analysis has ignored propagation loss and less-than-ideal overlap between electrical and optical fields. Potassium niobate, barium titanate, and lithium niobate have been found to be among the more desirable electrooptic materials. The use of dielectric buffer layers, several thousand Angstroms in thickness, has been found necessary to isolate the modulator el high dielectric constant, high strength materials such as potass Buffer layers, however, have been generally unnecessary when using permittivity and lower electroopt materials such as lithium niobate. ctrodes f rom electroopt ic um niobate. ound to be the lower c strength
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