Design of an optical gas sensor based on chalcogenide (ChG) glass platform in the mid-infrared for detection of CO2 and CO

IF 4.3 3区 材料科学 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC ACS Applied Electronic Materials Pub Date : 2024-09-19 DOI:10.1007/s11082-024-07486-1
Nouhaila Benkohaila, Nathalie Lorrain, Saida Bahsine, Fatima Lmai, Joel Charrier
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Abstract

In this work, a gas sensing system based on chalcogenide (ChG) glass platform in the mid-infrared (Mid-IR) region is modeled. The proposed gas sensing system composed of a linear tapers waveguide, ridge waveguide, a multimode interferometer (MMI) coupler and transducer arms. The components of the sensing system were simulated using FimmWave from Photon design. First, we determined the structural key parameters of the ridge waveguide that allow for single-mode propagation while maximizing the evanescent confinement field factor. The obtained results show that at the gas absorption wavelengths, \({\uplambda }_{{\text{CO}}_{2}}\)= 4.26 µm and \({\uplambda }_{\text{CO}}\)= 4.6 µm, the evanescent confinement field factor, reached 3.12% and 3.24%, respectively. For these operating wavelengths, a maximum transmission of 99.8% was achieved with a taper length of 450 µm. The footprint of the MMI coupler is 32 \(\times\) 9975 µm2. A Contrast of 16.6 dB and insertion losses of 2 dB and 2.87 dB were obtained at \({\uplambda }_{{\text{CO}}_{2}}\) = 4.26 µm and \({\uplambda }_{\text{CO}}\) = 4.6 µm respectively. The sensor performance was validated at 4.26 µm and 4.6 µm, respectively, giving a detection limit of 10.73 ppm for carbon dioxide (CO2) at 4.26 µm and 138 ppm for carbon monoxide (CO) at 4.6 µm. A sensitivity of 3.02 mW.L/mol and 0.12 mW. L/mol, was achieved at the wavelenghts of interset. The obtained results of the sensor by the optimizations of its components serve to enhance a gas sensing system based on chalcogenide (ChG) glass platform.

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设计一种基于中红外砷化镓(ChG)玻璃平台的光学气体传感器,用于检测 CO2 和 CO
在这项工作中,我们模拟了一种基于中红外(Mid-IR)区域的铬化玻璃(ChG)平台的气体传感系统。拟议的气体传感系统由线性锥形波导、脊波导、多模干涉仪(MMI)耦合器和换能器臂组成。我们使用 Photon design 公司的 FimmWave 对传感系统的各个组件进行了模拟。首先,我们确定了脊波导的结构关键参数,以实现单模传播,同时最大限度地提高蒸发约束场因子。结果表明,在气体吸收波长为 \({\uplambda }_{\text{CO}}_{2}}\)= 4.26 µm 和 \({\uplambda }_{\text{CO}}\)= 4.6 µm 时,蒸发约束场因子分别达到 3.12% 和 3.24%。对于这些工作波长,在锥形长度为 450 µm 时,最大传输率达到 99.8%。MMI 耦合器的占地面积为 9975 μm2。在 \({\uplambda }_{\text{CO}}_{2}\) = 4.26 µm 和 \({\uplambda }_{\text{CO}}\) = 4.6 µm 时,对比度为 16.6 dB,插入损耗分别为 2 dB 和 2.87 dB。传感器性能分别在 4.26 微米和 4.6 微米处得到验证,在 4.26 微米处二氧化碳 (CO2) 的检测限为 10.73 ppm,在 4.6 微米处一氧化碳 (CO) 的检测限为 138 ppm。灵敏度分别为 3.02 mW.L/mol 和 0.12 mW.L/mol 。L/mol 的灵敏度。该传感器通过优化其组件获得的结果有助于增强基于铬化镓(ChG)玻璃平台的气体传感系统。
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7.20
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4.30%
发文量
567
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