纳米金涂覆微纳光纤的倏逝场氨气检测研究

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. doi: 10.12086/oee.2021.200451
引用本文: 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. doi: 10.12086/oee.2021.200451
Zhang W J, Zeng X L, Yang A, et al. Research on evanescent field ammonia detection with gold-nanosphere coated microfibers[J]. Opto-Electron Eng, 2021, 48(9): 200451. doi: 10.12086/oee.2021.200451
Citation: Zhang W J, Zeng X L, Yang A, et al. Research on evanescent field ammonia detection with gold-nanosphere coated microfibers[J]. Opto-Electron Eng, 2021, 48(9): 200451. doi: 10.12086/oee.2021.200451

纳米金涂覆微纳光纤的倏逝场氨气检测研究

  • 基金项目:
    国家自然科学基金资助项目(91750108);上海市科学技术委员会资助项目(20JC1415700,16520720900);上海市高等学校特聘教授(东方学者)项目;高等学校学科创新引智计划(111)(D20031)资助
详细信息
    作者简介:
    *通讯作者: 曾祥龙(1977-),男,博士,教授,主要从事非线性超快光学、特种光纤及其传感技术的研究。E-mail:zenglong@shu.edu.cn
  • 中图分类号: TN248

Research on evanescent field ammonia detection with gold-nanosphere coated microfibers

  • Fund Project: National Natural Science Foundation of China (91750108), Science and Technology Commission of Shanghai Municipality (20JC1415700, 16520720900), and Program for Professor of Special Appointment (Eastern Scholar) at Shanghai Institutions of Higher Learning (111)(D20031)
More Information
  • 本文基于TDLAS技术,采用设计制备的微纳光纤气体吸收池,搭建了一套全光纤的NH3浓度检测系统。NH3检测系统的核心部分气体传感通过1.51 μm的微纳光纤完成,该系统检测结果表明,NH3在20000 ppm~100000 ppm浓度范围内,解调的二次谐波幅值与对应浓度之间具有良好的线性关系(拟合方程相关系数R=0.9962)。为了提高NH3浓度的检测性能,采用纳米金涂覆微纳光纤以增强光纤的倏逝场效应。根据实验结果,纳米金涂覆后的微纳光纤NH3浓度检测系统灵敏度有了很大提升,NH3浓度的检测下限可达到260 ppm。对不同浓度的NH3反复监测显示该检测系统稳定性良好,最大相对误差为5.38%,适用于长期稳定性的NH3监测,具有广泛的应用前景。

  • Overview: Tunable diode laser absorption spectroscopy (TDLAS) is a highly sensitive laser absorption spectrum measurement technology, which determines the information of target gas by detecting the absorption intensity of the spectrum. With high selectivity, high sensitivity, rapid detection and high precision, it has been widely used in the real-time and online detection of atmospheric trace and polluted gases. However, most of gas absorption cells used in the existing detection system are based on the reflected spatial light structure, which requires the cooperation of the collimator with high precision. The structure of gas absorption cells is complex, expensive and bulky. On the other side, the optical fiber gas sensor based on fiber evanescent field is a neoteric kind of technology, and thus it takes light to measure the signal of the carrier and can adapt to various environments. Moreover, the evanescent field based optical fiber by coating various nanomaterials can improve the sensitivity of gas sensing, which has attracted wide attention.

    In this paper, combined with TDLAS technology and gas sensing based on the evanescent field fiber, a set of all-fiber NH3 concentration detection system was built. The light source is a distributed feedback laser at around 1512 nm and the laser controller is modulated to select the unique absorption spectrum of NH3 to reduce the interference of carbon dioxide, vapor and other trace gases. A small gas absorption cell consists of a tapered microfiber with a 1.51 μm diameter. The microfiber was pulled into a cone by hydrogen and oxygen flame technology, and the second harmonic signal was finally extracted by a lock-in amplifier. The experimental results verified the feasibility of the evanescent field gas absorption cell, which is applied in the TDLAS system to detect ammonia gas. There was a good linear relationship between the amplitude of the second harmonic and the corresponding concentration in the range of 20000 ppm~100000 ppm of NH3. To improve the detection performance of NH3 concentration, gold-nanosphere (GNS) coated microfiber was used to enhance the effect of fiber evanescent fields. Compared with the measurement results of the evanescent field and GNSs coated microfiber, the detection sensitivity of the coated evanescent field significantly improved. Meanwhile, the TDLAS detection system based on GNSs coated microfibers as the evanescent-field based fiber gas absorption cell has good stability with the maximum relative error of 5.38%, and the detection limit of NH3 concentration can reach 260 ppm. The system has a wide application prospect in the field of ammonia detection.

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  • 图 1  CO2, H2O和NH3在1512 nm附近的吸收峰

    Figure 1.  Absorption peaks of CO2, H2O and NH3 nearly 1512 nm

    图 2  微纳光纤气体吸收池式TDLAS氨气检测系统示意图

    Figure 2.  The schematic diagram of the TDLAS ammonia detection system with a microfiber gas absorption cell

    图 3  激光器输出特性。(a) 驱动电流从30 mA至70 mA的激光器输出光谱,温度为25 ℃; (b) 激光器随工作温度的变化输出光谱,电流为50 mA; (c) 不同温度和不同电流时,输出波长对应曲线; (d) 不同驱动电流对应的激光器输出功率与加载电压

    Figure 3.  The characteristic of laser output. (a) The output spectrum of the laser when the driving current is adjusted from 30 mA to 70 mA, and the operating temperature is 25 ℃; (b) The output spectrum of laser with the change of working temperature, and the driving current is 50 mA; (c) The output wavelength corresponds to the curve at different temperature and current; (d) The output power and loading voltage of laser with different driving current

    图 4  (a) 微纳光纤结构图; (b) 微纳光纤拉制时间、锥区均匀区域直径与传输损耗之间的对应关系; (c) 微纳光纤直径

    Figure 4.  (a) The structure chart of a microfiber; (b) The relationship between drawing time, diameter of uniform region and transmission loss in the microfiber; (c) Diameter of the microfiber

    图 5  微纳光纤在(a) GNSs涂覆之前和(b) GNSs涂覆之后的倏逝场辐射; (c) 微纳光纤表面沉积GNSs的SEM图像,插入的是一段沉积GNSs的微纳光纤

    Figure 5.  The evanescent field radiation of the microfiber before (a) and after (b) GNSs deposition; (c) SEM image of the GNSs deposited on the surface of the microfiber. The insertion is a segment of the microfiber deposited by GNSs

    图 6  (a) 微纳光纤气体吸收池不同NH3浓度的二次谐波信号; (b) 二次谐波信号幅值与NH3浓度的实测数据和线性拟合曲线

    Figure 6.  (a) 2f signals at different NH3 concentrations; (b) The measured data and linear fitting curve of the 2f signal's amplitude versus NH3 concentration

    图 7  (a) GNSs涂覆后微纳光纤气体吸收池不同NH3浓度时的二次谐波信号; (b) 二次谐波信号幅值与NH3浓度的实测数据和线性拟合曲线; (c) 浓度为6000 ppm的NH3的吸收波形及其对应的二次谐波(小图为无吸收处的噪音)

    Figure 7.  (a) 2f signals at different NH3 concentrations in the microfiber gas absorption pool after GNSs coating; (b) The measured data and linear fitting curve of the 2f signal's amplitude versus NH3 concentration; (c) The absorption waveform of NH3 with concentration of 6000 ppm and its corresponding second harmonic wave (the small figure is the noise without absorption)

    表 1  系统稳定性测量结果

    Table 1.  The measurement results of system stability

    Serial number Amplitude/V True concentration/ppm Measured concentration/ppm Absolute error/ppm Relative error/%
    1 0.578 2000 1954 -46.15 -2.31
    2 0.582 2000 2107 107.69 5.38
    3 0.636 4000 4185 184.62 4.62
    4 0.628 4000 3877 -123.08 -3.08
    5 0.684 6000 6031 30.77 0.51
    6 0.690 6000 6262 261.54 4.36
    7 0.734 8000 7954 -46.15 -0.58
    8 0.730 8000 7800 -200 -2.50
    9 0.788 10000 10031 30.77 0.31
    10 0.796 10000 10338 388.46 3.38
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收稿日期:  2020-12-04
修回日期:  2021-07-15
刊出日期:  2021-09-15

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