基于基频和三次谐波瑞利波在ZnO/熔融二氧化硅中的传播的紫外传感器

C. Caliendo, D. Cannatà, M. Benetti, A. Buzzin
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引用次数: 1

摘要

采用射频反应磁控溅射技术在熔融二氧化硅衬底上生长了c轴取向的ZnO压电层。波长80 μm的金属交叉换能器光刻在4 μm厚的ZnO自由表面上,激发了基模、瑞利波及其谐波(第3次和第9次)的传播。在一定的紫外功率密度(365 nm)下,实验研究了紫外光吸附在光导氧化锌层中引起的声电效应,即波速变化。从ZnO/熔融二氧化硅衬底的顶表面或从ZnO层的后表面(通过熔融二氧化硅衬底)照射ZnO/熔融二氧化硅衬底,紫外功率值高达约0.45 W。在顶光(1044和2305 ppm/(mWcm-2)和背光(1084和2488 ppm/(mWcm-2)的基频和三谐波模式下,计算了传感器的灵敏度,即单位紫外功率密度的相对速度位移。三次谐波的谐振频率约为基模谐振频率的三倍,其灵敏度大于基模的灵敏度。在背光下测试的两个传感器的灵敏度都比在正面照明下测试的灵敏度大。九次谐波模式也被测试用于365 nm的紫外感应:它对紫外敏感,但由于该模式的高插入损耗(等于- 80 dB)远远大于基波和三次谐波模式(等于-62和-50 dB),其灵敏度无法以良好的精度测量。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
UV sensors based on the propagation of the fundamental and third harmonic Rayleigh waves in ZnO/fused silica
c-axis oriented piezoelectric ZnO layers were grown by rf reactive magnetron sputtering technique onto fused silica substrates. The propagation of the fundamental mode, the Rayleigh wave, and its harmonics (third and ninth) was excited by metal interdigitated transducers (80 μm wavelength) photolithographically implemented onto the free surface of the ZnO layer (4 μm thick). The acoustoelectric effect, the waves velocity changes induced by the UV light adsorption in the photoconductive ZnO layer, was experimentally investigated at some UV power densities 365 nm. The ZnO/fused silica substrates were illuminated from the top surface or from the back surface of the ZnO layer (through the fused silica substrate) for UV power values up to about 0.45 W. The sensors sensitivities, the relative velocity shift per unit UV power density, were calculated for the fundamental and third harmonic modes for top illumination (1044 and 2305 ppm/(mWcm-2) and for back illumination (1084 and 2488 ppm/(mWcm-2). The third harmonic wave, whose resonant frequency is about three times the resonant frequency of the fundamental mode, has sensitivity larger than that of the latter. Both the two sensors tested under back illumination have a sensitivity larger than that measured under front illumination. The ninth harmonic mode as well was tested for UV sensing at 365 nm: it is sensitive to UV but its sensitivity could not be measured with good accuracy due to the high insertion loss of the mode (equal to - 80 dB) which was much larger than that of the fundamental and third harmonic mode (equal to -62 and -50 dB).
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