Determination of the Paratellurite Stiffness Constants Temperature Coefficients by the Acousto-Optic Method

S. Mantsevich, E. Kostyleva
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引用次数: 2

Abstract

Acousto-optic (AO) phase matching condition is determined not only by the optical and acoustic waves propagation direction and parameters, but also by the physical characteristics of the AO interaction medium. Wherein, these characteristics, mainly the acoustic wave velocity, are temperature dependent. The change of ultrasound velocity relies on the medium stiffness constants cij variation with temperature. However, even for the most popular AO material – tellurium dioxide, the values of the stiffness constants temperature coefficients, given in various papers, vary significantly. The experimentally observed AO phase matching frequency temperature shift values do not coincide with those evaluated with literature data. In order to eliminate the observed discrepancy between theory and experiment, the AO phase matching frequency temperature dependencies for several AO cells based on TeO2 crystals with cut angles varying from 1.8° to 19° from the [110] axis in the (1‾10) plane were analyzed. The ultrasound velocity variation temperature coefficients were evaluated and the c11-c12 and c44 temperature coefficients that define the slow acoustic mode velocity in the selected plane were determined.
声光法测定副卫星刚度常数和温度系数
声光相位匹配条件不仅取决于光波和声波的传播方向和参数,还取决于声光相互作用介质的物理特性。其中,这些特性,主要是声波速度,与温度有关。超声声速的变化依赖于介质刚度常数随温度的变化。然而,即使是最常用的AO材料二氧化碲,在各种论文中给出的刚度常数温度系数值也有很大差异。实验观测到的AO相位匹配频率温移值与文献数据计算的值不一致。为了消除观察到的理论与实验之间的差异,分析了几种基于TeO2晶体的AO单元的AO相位匹配频率温度依赖关系,其切割角度在(1 - 10)平面上从[110]轴的1.8°到19°不等。计算了超声速度变化温度系数,确定了在选定平面内定义慢声模态速度的c11-c12和c44温度系数。
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