Sensing ultrasound optically with photonic crystal slabs: a tale of two mechanisms (Conference Presentation)

E. Zhu, C. Rewcastle, R. Gad, L. Qian, O. Levi
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引用次数: 0

Abstract

Silicon Photonics-based sensors can provide low cost, high sensitivity optical detection solutions in ultrasound and photoacoustic (PA) imaging. We demonstrate experimentally the measurement of ultrasound (2.5-8.5 MHz) in water using photonic crystal slab (PCS) nanostructure devices. Each PCS is composed of a periodic array of nanoholes, etched into silicon nitride (t=160 nm), on top of a silicon dioxide layer, and silicon substrate. The PCS devices have guided resonances that peak at ~ 1550 nm, with linewidths that vary from 0.7 to 5.5 nm. One type of PCS device includes a PCS nanostructure located above a thin micro-fabricated silicon membrane (~ 10 micron thick). Membrane deformation by incoming ultrasound waves induce resonance changes in the PCS spectral peak location (i.e., drum effect). We observe these drum-effect PCS devices to have acoustic sensitivities that are very narrowband (with bandwidths ~ 1 MHz), with a 300-micron diameter drum device found to have a peak sensitivity at 5 MHz and a noise equivalent pressure (NEP) of 2.0 kPa (72 Pa/rt Hz). In another mechanism, the sensitivity of the PCS nanostructures to changes in the ambient index of refraction is used. A pressure wave in water that impinges the PCS is accompanied by changes in the water's index of refraction, which causes the resonance peak of the PCS to shift. The acoustic sensitivities of these PCS devices is found to be broadband (> 6 MHz), in contrast to the drum-effect devices, with an NEP of less than 0.5 kPa (6.7 Pa/rt Hz). These devices can potentially allow for optics-based monolithic ultrasound sensor arrays, optimized for PA imaging.
光子晶体板的超声传感:两种机制的故事(会议报告)
基于硅光子学的传感器可以为超声和光声成像提供低成本、高灵敏度的光学检测解决方案。实验证明了利用光子晶体板(PCS)纳米结构器件测量水中超声波(2.5-8.5 MHz)。每个PCS都是由一个周期性的纳米孔阵列组成,蚀刻在氮化硅(t=160 nm)上,在二氧化硅层和硅衬底上。PCS器件的引导共振峰在~ 1550nm处,线宽从0.7到5.5 nm不等。一种类型的PCS器件包括位于薄微加工硅膜(~ 10微米厚)之上的PCS纳米结构。超声入射引起膜变形,引起PCS谱峰位置的共振变化(即鼓效应)。我们观察到这些鼓效应PCS器件具有非常窄带的声灵敏度(带宽约为1 MHz),其中300微米直径的鼓装置在5 MHz处具有峰值灵敏度,噪声等效压力(NEP)为2.0 kPa (72 Pa/rt Hz)。另一种机制是利用PCS纳米结构对环境折射率变化的敏感性。水中的压力波撞击到PCS时,会伴随着水的折射率变化,从而导致PCS的共振峰发生移位。与鼓效应装置相比,这些PCS装置的声灵敏度被发现是宽带的(> 6 MHz), NEP小于0.5 kPa (6.7 Pa/rt Hz)。这些设备可能允许基于光学的单片超声传感器阵列,优化了PA成像。
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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