基于非线性振荡的MEMS红外探测器和基于表面等离子激元的波长选择发射器

M. Sasaki, S. Kumagai
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引用次数: 1

摘要

悬浮式MEMS结构适用于减少热传导造成的能量损失。有可能红外光子能量可以很好地控制,以产生一些物理效应。提出了一种基于探测器非线性振荡的新方法。当挠曲发生在薄膜的面外方向时,薄膜扭转弹簧表现出较大的硬弹簧效应。当红外被吸收时,谐振腔由于热膨胀而弯曲。随着共振频率的增加,扭转弹簧变硬。频率测量适合于精密传感。使用激光(波长650nm)测量器件响应。谐振频率为88-94kHz。在真空(1Pa)下,Q因子约为1600。灵敏度为-0.144[kHz/(kW/m2)]。发射器采用非色散红外气体传感器。分子有其固有的吸收率。CO2吸收的波长为4.2 ~ 4.3μm。主要的白炽灯泡具有广谱发射红外,不用于气体传感。气体带宽处的波长选择性将提高效率。一种新的原理是将微加热器面向光栅放置。SPP在光栅表面携带红外能量被激发。红外发射是在输出端发生的反向激发过程。发射光谱显示SPP相关峰宽度为190nm。当输入功率从0.3 w增加到1.9W时,3.5μm波长处的峰值更加清晰。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
MEMS infrared approaches to detector based on nonlinear oscillation and wavelength selective emitter using surface plasmon polariton
The suspended MEMS structure is suitable for reducing the energy loss due to the thermal conduction. There is the possibility that IR photon energy can be well-controlled to generate some physical effects. A new method bases on the nonlinear oscillation for the detector. The thin film torsional spring exhibits a large hard spring effect when the deflection occurs in the out-of-plane direction of the film. When IR is absorbed, the resonator bends due to the thermal expansion. The torsional spring becomes harder increasing the resonant frequency. The frequency measurement is suited for the precise sensing. The device response is measured using the laser (wavelength of 650nm). The resonant frequency is 88-94kHz. Q factor is about 1600 in vacuum (1Pa). The sensitivity is -0.144[kHz/(kW/m2)]. As for the emitter, nondispersive IR gas sensor is considered. The molecules have their intrinsic absorptions. CO2 absorbs the wavelength 4.2- 4.3μm. The major incandescent light bulbs have the broad spectrum emitting IR which is not used for gas sensing. The wavelength selectivity at the gas bandwidth will improve the efficiency. A new principle uses the microheater placed facing to the grating. SPP is excited carrying IR energy on the grating surface. IR emission is the reverse process of excitation occurring at the output end. The emission spectra show SPP related peak having the width of 190nm. When the input power increases from 0.3 to 1.9W, the peak at wavelength of 3.5μm becomes clearer.
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