Multi-electrode array for spectral bandwidth control

J. Champagne, J. Kastelik, S. Dupont
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Abstract

Acousto-optical tunable filters (AOTFs) are well used for practical applications and are most often based on the classical anisotropic non-collinear configuration in tellurium dioxide crystals. Any product sheet of such a commercially available AOTF presents two main features: the tuning range and the spectral bandwidth Δλ. The spectral transmission bandwidth1 is proportional to the ratio λ2 /(bW) where λ is the optical wavelength, b the dispersive constant and W the length of the transducer. The dispersive constant b is a rapidly decreasing function of the wavelength in the blue visible spectrum. As for examples: for a one octave tuning range starting from 400 nm to 800 nm, the spectral bandwidth is multiplied by ~10. For a tuning range in the infrared band 1250-2500 nm, the spectral bandwidth is multiplied by ~4. We present the design of a filter operating in the visible region from 450 nm to 650 nm. A double anisotropic interaction2 is considered allowing the simultaneous diffraction of the two optical modes propagating into the crystal by a single ultrasonic wave. A multi-electrode array of three identical consecutive electrodes Wi:1-3 = 3 mm is deposited on the transducer leading to a more precise control of the spectral bandwidth. The acousto-optic device has been fabricated by the AA-Opto company. With this component the spectral bandwidth is only multiplied by ~2 on from 400 nm to 650 nm.
用于频谱带宽控制的多电极阵列
声光可调谐滤波器(AOTFs)在实际应用中得到了很好的应用,并且通常基于二氧化碲晶体中的经典各向异性非共线结构。这种商用AOTF的任何产品表都具有两个主要特征:调谐范围和频谱带宽Δλ。光谱传输带宽1与λ2 /(bW)成正比,其中λ为光波长,b为色散常数,W为换能器长度。色散常数b是蓝色可见光谱中波长的速降函数。例如:对于从400nm到800nm的一倍频的调谐范围,频谱带宽乘以~10。在红外波段1250 ~ 2500nm的调谐范围内,光谱带宽乘以~4。我们设计了一种工作在450 nm到650 nm可见光区域的滤波器。双各向异性相互作用2被认为允许两种光学模式同时衍射传播到晶体通过一个单一的超声波。三个相同的连续电极Wi:1-3 = 3mm的多电极阵列沉积在换能器上,从而更精确地控制光谱带宽。声光器件由AA-Opto公司制造。使用该组件,光谱带宽仅在400nm到650nm之间乘以2倍。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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