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用于掩埋氮化硅波导中声光调制的表面声波

Surface acoustic waves for acousto-optic modulation in buried silicon nitride waveguides.

作者信息

van der Slot Peter J M, Porcel Marco A G, Boller Klaus-J

出版信息

Opt Express. 2019 Jan 21;27(2):1433-1452. doi: 10.1364/OE.27.001433.

Abstract

We theoretically investigate the use of Rayleigh surface acoustic waves (SAWs) for refractive index modulation in optical waveguides consisting of amorphous dielectrics. Considering low-loss SiN waveguides with a standard core cross-section of 4.4×0.03 μm size, buried 8-μm deep in a SiO cladding, we compare surface acoustic wave generation in various different geometries via a piezo-active, lead zirconate titanate film placed on top of the surface and driven via an interdigitized transducer (IDT). Using numerical solutions of the acoustic and optical wave equations, we determine the strain distribution of the SAW under resonant excitation. From the overlap of the acoustic strain field with the optical mode field, we calculate and maximize the attainable amplitude of index modulation in the waveguide. For the example of a near-infrared wavelength of 840 nm, a maximum shift in relative effective refractive index of 0.7x10 was obtained for TE polarized light, using an IDT period of 30-35 μm, a film thickness of 2.5-3.5 μm, and an IDT voltage of 10 V. For these parameters, the resonant frequency is in the range of 70-85 MHz. The maximum shift increases to 1.2x10, with a corresponding resonant frequency of 87 MHz, when the height of the cladding above the core is reduced to 3 μm. The relative index change is about 300 times higher than in previous work based on non-resonant proximity piezo-actuation, and the modulation frequency is about 200 times higher. Exploiting the maximum relative index change of 1.2×10 in a low-loss, balanced Mach-Zehnder modulator should allow full-contrast modulation in devices as short as 120 μm (half-wave voltage length product = 0.24 Vcm).

摘要

我们从理论上研究了利用瑞利表面声波(SAW)对由非晶电介质构成的光波导中的折射率进行调制。考虑到具有4.4×0.03μm标准芯部横截面、埋入8μm深的SiO包层中的低损耗SiN光波导,我们通过放置在表面顶部并由叉指换能器(IDT)驱动的压电活性锆钛酸铅薄膜,比较了各种不同几何结构中表面声波的产生情况。利用声波和光波方程的数值解,我们确定了共振激发下SAW的应变分布。根据声应变场与光学模场的重叠情况,我们计算并最大化了光波导中可实现的折射率调制幅度。以840nm的近红外波长为例,对于TE偏振光,使用30 - 35μm的IDT周期、2.5 - 3.5μm的薄膜厚度和10V的IDT电压,相对有效折射率的最大变化为0.7×10⁻⁴。对于这些参数,共振频率在70 - 85MHz范围内。当芯部上方包层的高度减小到3μm时,最大变化增加到1.2×10⁻⁴,相应的共振频率为87MHz。相对折射率变化比基于非共振近场压电驱动的先前工作高约300倍,调制频率高约200倍。在低损耗、平衡马赫曾德尔调制器中利用1.2×10⁻⁴的最大相对折射率变化,应能在短至120μm(半波电压长度积 = 0.24V·cm)的器件中实现全对比度调制。

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