TDLAS气体遥测高灵敏光电探测电路设计 -

姓名
邮箱
手机号码
标题
留言内容
验证码

TDLAS气体遥测高灵敏光电探测电路设计

doi:10.37188/CO.2023-0107

裴梓伊^{1, 2,},
胡朋兵^{2, 3},
潘孙强^{2, 3},
戚海洋^{2, 3},
刘素梅^{2, 3},
刘东^1,,

1.
浙江大学光电科学与工程学院极端光学技术与仪器全国重点实验室, 浙江杭州310027
2.
浙江省计量科学研究院, 浙江杭州310018
3.
浙江省能源与环境保护计量检测重点实验室, 浙江杭州310018

基金项目:2022 年度“尖兵”“领雁”研发攻关计划项目（2022C03065，2022C03162，2022C03084）；浙江省市场监督管理局雏鹰计划培育项目（CY2023001）；浙江省市场监督管理局科研计划项目（QN2023419）

详细信息

作者简介:
裴梓伊（1998—），男，辽宁葫芦岛人，硕士研究生在读，2021年于哈尔滨工业大学获得学士学位，主要研究方向为光学检测技术。E-mail:ziyipei@zju.edu.cn
刘东（1982—），男，辽宁大连人，教授，博士，博士生导师，分别于2005年和2010年在浙江大学获得学士和博士学位，曾在美国宇航局(NASA)从事博士后研究工作。主要研究方向为光学检测、雷达、机器视觉、深度学习。E-mail：liudongopt@zju.edu.cn

中图分类号:O433.1；O433.4
计量
- 文章访问数:16
- HTML全文浏览量:2
- PDF下载量:6
- 被引次数:0
出版历程
- 网络出版日期:2023-11-23

Design of a Highly Sensitive Photoelectric Detection Circuit for TDLAS Gas Laser Telemetry

PEI Zi-yi^{1, 2,},
HU Peng-bing^{2, 3},
PAN Sun-qiang^{2, 3},
QI Hai-yang^{2, 3},
LIU Su-mei^{2, 3},
LIU Dong^1,,

1.
State Key Laboratory of Modern Optical Instrumentation, College of Optical Science and Engineering, Zhejiang University, Hangzhou 310027, China
2.
Zhejiang Institute of Metrology, Hangzhou 310018, China
3.
Key Laboratory of Energy and Environmental Protection Measurement of Zhejiang Province, Hangzhou 310018, China

Funds:Supported by the“Pioneer” and “Leading Goose” R&D Program of Zhejiang (No. 2022C03065，2022C03162，2022C03084). Science and Technology Plan Program, Eagle Plan Training Program of Marketing Surveillance & Administration Bureau of Zhejiang Province (No. QN2023419, No. CY2023001).

More Information

Corresponding author:liudongopt@zju.edu.cn

摘要

摘要:
针对气体遥测光信号微弱、环境因素干扰强等特点，结合波长调制技术，设计和研究了用于TDLAS 遥测的高灵敏度光电探测电路(High Sensitivity Photoelectric Detection Circuit, HSPDC)。基于波长调制技术，确定了TDLAS信号噪声抑制方法；采用光电二极管理想模型，分析了光电探测电路线性响应特性并确定了光电二极管的关键参数；基于级联放大原理设计仿真并测试了HSPDC，光功率检测下限0.11 nW，信号衰减仅为0.79 dB(f=10 kHz)，截止频率高于现有10⁸V/A跨阻放大电路一个数量级，可用于高速调制微弱光信号的探测。搭建了气体遥测系统，当调制频率为3 kHz时，遥测系统获得了良好的检测性能，检测灵敏度达到88.66 mV/ppm，检测限优于0.565 ppm，线性拟合度R²为0.9996。研究表明，研制的HSPDC光电探测电路具有响应速度快、检测灵敏度和等优点，可集成化，能满足气体遥测应用需求。
- 光电探测/
- 跨阻放大/
- TDLAS/
- 开放光路/
- 遥测.
Abstract:
To address weak gas laser telemetry optical signals and strong interference from environmental factors, a Highly Sensitive Photoelectric Detection Circuit (HSPDC) for TDLAS laser telemetry has been designed and investigated using wavelength modulation technology. In addition, Furthermore, a noise suppression method for TDLAS signals based on this technology was determined. The photodiode ideal model is utilized to analyze the linear response characteristics of the photodetector circuit and determine the essential photodiode parameters. Based on the cascade amplification principle, the HSPDC is designed, simulated, and tested, achieving a lower limit of optical power detection of 0.11 nW, a signal attenuation of 0.79 dB (f=10 kHz). The cutoff frequency is one order of magnitude higher than the existing 108 V/A cross-impedance amplification circuit. Therefore, HSPDC is applicable for high-speed modulation of weak optical signals. The laser telemetry system exhibits excellent detection performance at a modulation frequency of 3 kHz, with a detection sensitivity of 88.66 mV/ppm, a detection limit of less than 0.565 ppm, and a linear fit R²of 0.9996. The study demonstrates that the HSPDC photoelectric detection circuit offers the advantages of fast response, high detection sensitivity and accuracy, rendering it ideal for gas laser telemetry applications.
- photoelectric detection/
- transimpedance amplification/
- TDLAS/
- ppen light path/
- laser telemetry

HTML全文

图 1各次谐波信号(a)奇次谐波信号(b)偶次谐波信号

Figure 1.Each harmonic signal (a) odd harmonic signal (b) even harmonic signal

下载: 全尺寸图片幻灯片

图 2PIN 光电二极管等效模型

Figure 2.Equivalent model of PIN photodiode

下载: 全尺寸图片幻灯片

图 3I—I_L响应关系(a)R_d=10 kΩ (b)R_d=100 kΩ (c)R_d=1 MΩ

Figure 3.I—I_Lresponse relationship (a)R_d=10 kΩ (b)R_d=100 kΩ (c)R_d=1 MΩ

下载: 全尺寸图片幻灯片

图 4光电探测电路原理示意图(a) 跨阻放大电路(b) 负反馈放大电路(c) BW滤波电路

Figure 4.Schematic diagram of photoelectric detection circuit (a) cross resistance amplification circuit (b) negative feedback amplification circuit (c) BW filtering circuit

下载: 全尺寸图片幻灯片

图 5光电探测电路仿真(a) 各级放大电路输出信号(b) 增益及相位频率响应特性

Figure 5.Photoelectric detection circuit simulation (a) output signal of each stage of amplification circuit (b) gain and phase vs.frequency response characteristic

下载: 全尺寸图片幻灯片

图 6氨气遥测系统结构示意图

Figure 6.Schematic diagram of ammonia laser telemetry structure

下载: 全尺寸图片幻灯片

图 7暗电流噪声信号(a) HSPDC 噪声(b) TLB PDC 噪声

Figure 7.Dark current noise signal (a) HSPDC noise (b) TLB PDC noise

下载: 全尺寸图片幻灯片

图 8遥测距离变化时系统输出信号(a) HSPDC 输出信号(b) TLB PDC 输出信号

Figure 8.System output signal when telemetry distance changes (a) HSPDC output signal (b) TLB PDC output signal

下载: 全尺寸图片幻灯片

图 9二次谐波峰峰值及标准偏差随距离变化曲线

Figure 9.Curves of the peak value of the second harmonic peak and standard deviation as a function of distance

下载: 全尺寸图片幻灯片

图 10二次谐波峰峰值随调制频率影响曲线

Figure 10.The curve of the peak value of the second harmonic peak as a function of the modulation frequency influence

下载: 全尺寸图片幻灯片

图 11系统输出二次谐波波形(a) 气体浓度0.2% (b) 气体浓度1% (c) 气体浓度2%

Figure 11.System output second harmonic waveform (a) gas concentration 0.2% (b) gas concentration 1% (c) gas concentration

下载: 全尺寸图片幻灯片

图 12调制信号为 1 kHz和 3 kHz时系统浓度响应特性曲线

Figure 12.System concentration response characteristic curve when modulation signals are 1 kHz and 3 kHz

下载: 全尺寸图片幻灯片

参考文献 (28)

[1]	YU S F, ZHANG ZH, XIA H Y,et al. Photon-counting distributed free-space spectroscopy[J].Light:Science & Applications, 2021, 10(1): 212.
[2]	CHEN S J, TONG B W, RUSSELL L M,et al. Lidar-based daytime boundary layer height variation and impact on the regional satellite-based PM_2.5estimate[J].Remote Sensing of Environment, 2022, 291: 113224.
[3]	XIAO D, WANG N CH, CHEN S J,et al. Simultaneous profiling of dust aerosol mass concentration and optical properties with polarized high-spectral-resolution lidar[J].Science of the Total Environment, 2023, 872: 162091.doi:10.1016/j.scitotenv.2023.162091
[4]	ZHANG K, CHEN Y T, ZHAO H K,et al. Comprehensive, continuous, and vertical measurements of seawater constituents with triple-field-of-view high-spectral-resolution lidar[J].Research, 2023, 6: 0201.doi:10.34133/research.0201
[5]	WANG N CH, ZHANG K, SHEN X,et al. Dual-field-of-view high-spectral-resolution lidar: Simultaneous profiling of aerosol and water cloud to study aerosol-cloud interaction[J].Proceedings of the National Academy of Sciences of the United States of America, 2022, 119(10): e2110756119.
[6]	KE J, SUN Y SH, DONG CH ZH,et al. Development of China’s first space-borne aerosol-cloud high-spectral-resolution lidar: retrieval algorithm and airborne demonstration[J].PhotoniX, 2022, 3: 17.doi:10.1186/s43074-022-00063-3
[7]	WEN L, SUN ZH W, ZHENG Q Let al. On-chip ultrasensitive and rapid hydrogen sensing based on plasmon-induced hot electron–molecule interaction[J].Light:Science & Applications, 2023, 12: 76.
[8]	WU L M, YUAN X X, TANG Y X,et al. MXene sensors based on optical and electrical sensing signals: from biological, chemical, and physical sensing to emerging intelligent and bionic devices[J].PhotoniX, 2023, 4(1): 15.doi:10.1186/s43074-023-00091-7
[9]	LEE J, YU E S, KIM T,et al. Naked-eye observation of water-forming reaction on palladium etalon: transduction of gas-matter reaction into light-matter interaction[J].PhotoniX, 2023, 4(1): 20.doi:10.1186/s43074-023-00097-1
[10]	ZHANG CH X, LIU CH, HU Q H,et al. Satellite UV-Vis spectroscopy: implications for air quality trends and their driving forces in China during 2005-2017[J].Light:Science & Applications, 2021, 8: 100.
[11]	VLK M, DATTA A, ALBERTI S,et al. Extraordinary evanescent field confinement waveguide sensor for mid-infrared trace gas spectroscopy[J].Light:Science & Applications, 2021, 10(1): 26.
[12]	DENG Y, FAN ZH F, ZHAO B B,et al. Mid-infrared hyperchaos of interband cascade lasers[J].Light:Science & Applications, 2021, 11(1): 7.
[13]	MARINOV E, MARTINS R J, YOUSSEF M A B,et al. Overcoming the limitations of 3D sensors with wide field of view metasurface-enhanced scanning lidar[J].Advanced Photonics, 2023, 5(4): 046005.
[14]	HUANG ZH T, CHANG C Y, CHEN K P,et al. Tunable lasing direction in one-dimensional suspended high-contrast grating using bound states in the continuum[J].Advanced Photonics, 2022, 4(6): 066004.
[15]	张志荣, 夏滑, 孙鹏帅, 等. 基于高灵敏吸收光谱技术的稳定气态同位素测量及其应用(特邀)[J]. 光子学报,2023,52(3):0352108.doi:10.3788/gzxb20235203.0352108 ZHANG ZH R, XIA H, SUN P SH,et al. Stable gaseous isotope measurement method based on highly sensitive laser absorption spectroscopy and its applications (invited)[J].Acta Photonica Sinica, 2023, 52(3): 0352108. (in Chinese).doi:10.3788/gzxb20235203.0352108
[16]	钟笠, 宋迪, 焦月, 等. 具有复杂光谱特征的丙烯气体的TDLAS检测技术研究[J]. 中国光学,2020,13(5):1044-1054.doi:10.37188/CO.2019-0203 ZHONG L, SONG D, JIAO Y,et al. TDLAS detection of propylene with complex spectral features[J].Chinese Optics, 2020, 13(5): 1044-1054. (in Chinese).doi:10.37188/CO.2019-0203
[17]	张伟建, 曾祥龙, 杨傲, 等. 纳米金涂覆微纳光纤的倏逝场氨气检测研究[J]. 光电工程,2021,48(9):200451. ZHANG W J, ZENG X L, YANG A,et al. Research on evanescent field ammonia detection with gold-nanosphere coated microfibers[J].Opto-Electronic Engineering, 2021, 48(9): 200451. (in Chinese).
[18]	姚路, 刘文清, 刘建国, 等. 基于TDLAS的长光程环境大气痕量CO监测方法研究[J]. 中国 ,2015,42(2):0215003.doi:10.3788/CJL201542.0215003 YAO L, LIU W Q, LIU J G,et al. Research on open-path detection for atmospheric trace gas CO based on TDLAS[J].Chinese Journal of Lasers, 2015, 42(2): 0215003. (in Chinese).doi:10.3788/CJL201542.0215003
[19]	XIN F X, LI J, GUO J J,et al. Measurement of atmospheric CO₂column concentrations based on open-path TDLAS[J].Sensors, 2021, 21(5): 1722.doi:10.3390/s21051722
[20]	REN L, WANG X CH, HUANG G R,et al. Contribution of microchannel plate luminescence to the noise of 20-inch photomultiplier tubes[J].Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2022, 1022: 165973.
[21]	SUZUKI S, NAMEKATA N, TSUJINO K,et al. Highly enhanced avalanche probability using sinusoidally-gated silicon avalanche photodiode[J].Applied Physics Letters, 2014, 104(4): 041105.doi:10.1063/1.4861645
[22]	顾宇强, 谭明, 吴渊渊, 等. 具有优化倍增层InAlAs/InGaAs雪崩光电二极管[J]. 红外与毫米波学报,2021,40(6):715-720. GU Y Q, TAN M, WU Y Y,et al. InAlAs/InGaAs avalanche photodiode with an optimized multiplication layer[J].J. Infrared Millim. Waves, 2021, 40(6): 715-720. (in Chinese).
[23]	杨舒涵, 乔顺达, 林殿阳, 等. 基于可调谐半导体吸收光谱的氧气浓度高灵敏度检测研究[J]. 中国光学(中英文),2023,16(1):151-157.doi:10.37188/CO.2022-0029 YANG SH H, QIAO SH D, LIN D Y,et al. Research on highly sensitive detection of oxygen concentrations based on tunable diode laser absorption spectroscopy[J].Chinese Optics, 2023, 16(1): 151-157. (in Chinese).doi:10.37188/CO.2022-0029
[24]	王彪, 鹿洪飞, 李奥奇, 等. 采用VCSEL 光源的TDLAS甲烷检测系统的研制[J]. 红外与工程,2020,49(4):0405002.doi:10.3788/IRLA202049.0405002 WANG B, LU H F, LI A Q,et al. Research of TDLAS methane detection system using VCSEL laser as the light source[J].Infrared and Laser Engineering, 2020, 49(4): 0405002. (in Chinese).doi:10.3788/IRLA202049.0405002
[25]	CIURA Ł, KOLEK A, GAWRON W,et al. Measurements of low frequency noise of infrared photo-detectors with transimpedance detection system[J].Metrology and Measurement Systems, 2014, 21(3): 461-472.doi:10.2478/mms-2014-0039
[26]	梁万国, 罗森林, 周思永, 等. 光电探测器的设计[J]. 半导体光电,1998,19(1):52-56.doi:10.16818/j.issn1001-5868.1998.01.015 LIANG W G, LUO S L, ZHOU S Y,et al. Design of photodetector[J].Semiconductor Optoelectronics, 1998, 19(1): 52-56. (in Chinese).doi:10.16818/j.issn1001-5868.1998.01.015
[27]	Nicodemus F E, Richmond J C, Hsia J J,et al. Geometrical considerations and nomenclature for reflectance[EB/OL]. (1977-01-01).https://www.nist.gov/publications/geometrical-considerations-and-nomenclature-reflectance.(查阅网上资料,文献类型和内容不确定是否正确,请确认). Nicodemus F E, Richmond J C, Hsia J J,et al. Geometrical considerations and nomenclature for reflectance[EB/OL]. (1977-01-01).https://www.nist.gov/publications/geometrical-considerations-and-nomenclature-reflectance.(查阅网上资料,文献类型和内容不确定是否正确,请确认).
[28]	张雷雷, 曹振松, 钟磬, 等. FPGA主控型数字锁相放大器设计及光谱测量[J]. 红外与工程,2023,52(10):20230023. ZHANG L L, CAO Z S, ZHONG Q,et al. Digital lock-in amplifier controlled by FPGA for spectral measurement[J].Infrared and Laser Engineering, 2023, 52(10): 20230023.