基于紫外激光的羟基-平面激光诱导荧光探测研究进展

张仲磷; 杨岸龙; 王江; 程光华

doi:10.37188/CO.2024-0013

基于紫外激光的羟基-平面激光诱导荧光探测研究进展

doi: 10.37188/CO.2024-0013

1.
西北工业大学光电与智能研究院, 陕西西安 710072
2.
西安航天动力研究所, 陕西西安 710025

基金项目: 国家重点研发计划（No. 2022YFB4600201）

详细信息

作者简介:
张仲磷（1996—），男，甘肃定西人，西北工业大学博士研究生，2018年于西安电子科技大学获得学士学位，2020年于哈尔滨工程大学获得硕士学位，主要从事固体激光器设计方面的研究。E-mail：zhangzhonglin@mail.nwpu.edu.cn

程光华（1976—），男，陕西安康人，博士，教授，博士生导师，1999年于西北大学获得学士学位，2004年于中国科学院西安光学精密机械研究所获博士学位。主要从事超短脉冲激光技术、超快激光于物质相互作用、飞秒激光微纳加工技术研究。E-mail：guanghuacheng@nwpu.edu.cn

中图分类号: TP394.1;TH691.9
计量
- 文章访问数: 28
- HTML全文浏览量: 14
- PDF下载量: 3
- 被引次数: 0
出版历程
- 收稿日期: 2024-01-15
- 录用日期: 2024-03-25
- 网络出版日期: 2024-04-13

Research progress of hydroxy-plane laser induced fluorescence detection based on ultraviolet laser

1.
School of Artificial Intelligence, Optics and Electronics, Northwestern Polytechnical University, Xi’an 710072, China
2.
Science and Technology on Liquid Rocket Engine Laboratory, Xi’an Aerospace Propulsion Institute, Xi’an 710100, China

Funds: Supported by National Key Research and Development Program of China (No. 2022YFB4600201)

摘要

摘要:
羟基(OH)是一种广泛存在于燃烧反应过程中的产物，在燃烧诊断技术中，基于羟基的二维空间分布常用于表征火焰的锋面结构，同时羟基是表征火焰温度、火焰面密度和热释放速率等特征的重要参数。对燃烧火焰中的羟基进行有效探测是探究燃烧动力学演变过程，揭示火焰随机事件产生机理的重要支撑。平面激光诱导荧光(PLIF)技术作为一种光学测量方法具有时空分辨率高、无干扰、组份选择等优点，已成功对本生灯火焰、湍流火焰、旋流火焰和超声速火焰等多种燃烧火焰进行了结构观测，为建立燃烧模型提供了重要参考。本文从PLIF探测的基本原理开始，梳理了PLIF技术在燃烧诊断领域的发展历程和研究现状，介绍了基于染料激光、光参量振荡和钛宝石三倍频方式实现的PLIF紫外光源技术，并对不同技术路线的特点进行了讨论，最后对用于OH-PLIF的紫外激光技术发展进行了展望。
- 燃烧 /
- 平面激光诱导荧光 /
- 激光 /
- 羟基
Abstract:
Hydroxyl (OH) is a widely existing product in the combustion reaction process. In the combustion diagnosis technology, the two-dimensional spatial distribution based on hydroxyl is commonly used to characterize the structure of the flame front, while hydroxyl is an important parameter to characterize features such as the flame temperature, flame surface density, and heat release rate. The effective detection of hydroxyl in combustion flame is an important support for exploring the evolution of combustion dynamics and revealing the mechanism of random flame events. Planar laser-induced fluorescence (PLIF), as an optical measurement method, has the advantages of high spatial and temporal resolution, nonintrusive nature, and selection of components, and has successfully observed the structure of various combustion flames, such as Bunsen burner flame, turbulent flame, swirl flame and supersonic flame, which provides an important reference for the establishment of combustion models. This paper starts with the basic principle of PLIF detection, reviews the development history and research status of PLIF technology in the field of combustion diagnosis, introduces the PLIF ultraviolet light source technology based on dye laser, optical parametric oscillation and Ti:sapphire tripling-frequency, and discusses the characteristics of different technical routes. Finally, the development of UV laser technology for OH-PLIF is prospected.
- combustion /
- planar laser-induced fluorescence /
- laser /
- Hydroxyl

HTML全文

图 1 平面激光诱导荧光成像原理图

Figure 1. Schematic diagram of planar laser induced fluorescence imaging

下载: 全尺寸图片幻灯片

图 2 (a)平均速度矢量 (b)OH-PLIF探测结果^[29]

Figure 2. Mean velocity vectors (b) instantaneous OH-PLIF image^[29]

下载: 全尺寸图片幻灯片

图 3 丙酮-PLIF在旋转爆震发动机的径向图^[30]

Figure 3. Radial diagram of acetone-PLIF in a rotating detonation engine^[30]

下载: 全尺寸图片幻灯片

图 4 OH与CH-PLIF在流向截面的火焰结构成像对比^[33]

Figure 4. Comparison of OH-PLIF and CH-PLIF image in a cavity-stabilized scramjet combustor^[33]

下载: 全尺寸图片幻灯片

图 5 1-8个大气压贫预混天然气火焰OH测量^[18]

Figure 5. Experimental set-up for OH measurement of 1-8 atmospheres lean premixed natural gas flames^[18]

下载: 全尺寸图片幻灯片

图 6 (a)实验装置, (b)射流燃烧器, (c)成像区域^[44]

Figure 6. (a) Experimental setup, (b) jet burner, and (c) imaging region^[44]

下载: 全尺寸图片幻灯片

图 7 50 kHz高速OH-PLIF系统^[47]

Figure 7. 50 kHz high-speed OH-PLIF system^[47]

下载: 全尺寸图片幻灯片

图 8 20 kHz、CH₂O -PLIF/PIV实验装置^[48]

Figure 8. 20 kHz H, CH2O -PLIF/PIV experimental setup^[48]

下载: 全尺寸图片幻灯片

图 9 7.5 kHz、OH/CH₂O -PLIF实验装置^[50]

Figure 9. 7.5 kHz, OH/CH2O -PLIF experimental setup^[50]

下载: 全尺寸图片幻灯片

图 10 10 kHz 双平面PIV和OH-PLIF实验装置图^[51]

Figure 10. Diagram of the 10 kHz biplane PIV and OH-PLIF experimental setups^[51]

下载: 全尺寸图片幻灯片

图 11 OPO紫外激光实验装置^[52]

Figure 11. OPO Ultraviolet Laser Experimental Equipment^[52]

下载: 全尺寸图片幻灯片

图 12 种子注入burst模式OPO紫外激光实验装置^[53]

Figure 12. Experimental setup for seed injection of burst-mode OPO UV lasers^[53]

下载: 全尺寸图片幻灯片

图 13 基于OPO和倍频方式的50 kHz重频PLIF实验装置^[54]

Figure 13. Experimental setup for 50 kHz PLIF based on OPO and frequency doubling method^[54]

下载: 全尺寸图片幻灯片

图 14 超高速OH/CH₂O-PLIF探测系统^[55]

Figure 14. Schematic diagram of experimental setup for ultra-high-speed simultaneous OH and CH₂O-PLIF^[55]

下载: 全尺寸图片幻灯片

图 15 三臂Burst模式激光系统^[56]

Figure 15. Schematic of the three-legged burst-mode laser system^[56]

下载: 全尺寸图片幻灯片

图 16 (1) MHz泵浦源光路^[57] (2)(a)基于OPO-burst OH-PLIF的旋转爆震燃烧实验装置 (b)OPO光路图^[58]

Figure 16. (1) MHz pump source optical path ^[57] (2) (a) OPO-burst OH-PLIF based rotary burst combustion experimental setup (b) OPO optical path diagram^[58]

下载: 全尺寸图片幻灯片

图 17 飞秒OH-PLIF探测装置^[59]

Figure 17. Femtosecond OH-PLIF detector^[59]

下载: 全尺寸图片幻灯片

图 18 (1)基于钛宝石三倍频实现的283 nm紫外激光器(2)本生灯探测结果^[60]

Figure 18. (1) 283 nm UV laser based on titanium gemstone triplex realisation (2) Bunsen burner detection results^[60]

下载: 全尺寸图片幻灯片

表 1 用于OH-PLIF的紫外激光器性能对比

Table 1. Performance Comparison of UV Lasers for OH-PLIF

Year	Operation mode	Repetition frequency	Wavelength	Output power	Pulse energy	Conversion efficiency
2007^[18]	Rhodamine +SHG	10 Hz	283.92 nm	0.06 W	6 mJ	-
2007^[43]	Rhodamine 5G+BBO SHG	2.5 kHz 5 kHz	283 nm	130 mW 110 mW	50 μJ 22 μJ	0.7% 0.6%
2009^[44]	Rhodamine 6G+SHG	1.5 kHz	283 nm	0.82 W	0.54 mJ	1.6%
2009^[45]	Rhodamine 6G+BBO SHG	5 kHz	283.2 nm	0.5 W	100 μJ	2.6%
2010^[46]	Rhodamine 6G+BBO SHG	10 kHz	283.2 nm	1.4 W	140 μJ	3.5%
2014^[47]	Rhodamine 6G+2*BBO SHG+MOPA	50 kHz	283 nm	7 W	0.14 mJ	3.5%
2018^[48]	Burst/Rhodamine 6G+SHG	20 kHz	283	1.8 W	90 μJ	2.8%
2018^[49]	Burst/Rhodamine 6G+MOPA+BBO SHG	7.5 kHz	282.985 nm	16.5 W	2.2 mJ	-
2018^[11]	Rhodamine 590+SHG	-	283 nm	-	12 mJ	-
2020^[51]	Dye laser+SHG	10 kHz	283.9 nm	1.6 W	0.16 mJ	-
2009^[52]	Burst/Seeding OPO+BBO SHG	-	282.97 nm	0.2 W	-	-
2017^[53]	Burst/Seeding OPO+BBO SFG	10 kHz	284.005 nm	-	3 mJ	-
2017^[54]	Burst/Multi-YAG+OPO+SHG	50 kHz	283 nm	-	2 mJ	1.25%
2017^[55]	Burst/OPO+BBO SHG	50 kHz	284 nm	-	350 μJ	0.7%
2018^[56]	OPO+SFG	10 kHz	284 nm	-	5 mJ	0.7%
2020^[58]	Burst/Seeding OPO+BBO SFG	1 MHz	284 nm	-	400 μJ	0.6%
2020^[59]	fs Ti:sapphire+ BBO THG	1 kHz	283 nm	-	90 μJ	4.5%
2023^[60]	ns Ti:sapphire+LBO SHG+BBO THG	1 kHz	283 nm	0.56W	0.56 mJ	2.8%

下载: 导出CSV

参考文献(61)

[1]	武国华, 于欣, 彭江波, 等. 超燃冲压发动机羟基/煤油-PLIF同步测量研究[J]. 推进技术,2024,45(1):2210098. WU G H, YU X, PENG J B, et al. Simultaneous measurements of OH/Kerosene-PLIF in scramjet[J]. Journal of Propulsion Technology, 2024, 45(1): 2210098. (in Chinese).
[2]	JOO S, KWAK S, LEE M C. Effect of fuel line acoustics on the flame dynamics of H₂/CH₄ syngas in a partially premixed gas turbine combustor[J]. Fuel, 2021, 285: 119231. doi: 10.1016/j.fuel.2020.119231
[3]	尚勇, 何旭, 刘福水, 等. 燃烧光学可视化技术在内燃机测试中的应用研究[J]. 小型内燃机与车辆技术,2016,45(5):1-7. doi: 10.3969/j.issn.1671-0630.2016.05.001 SHANG Y, HE X, LIU F SH, et al. Research on the application of combustion optical visualization technology in the test of internal combustion engine[J]. Small Internal Combustion Engine and Vehicle Technique, 2016, 45(5): 1-7. (in Chinese). doi: 10.3969/j.issn.1671-0630.2016.05.001
[4]	王健儒, 晁侃, 陆贺建. 大型分段式固体火箭发动机点火瞬态过程研究[J]. 固体火箭技术,2017,40(2):141-145. doi: 10.7673/j.issn.1006-2793.2017.02.002 WANG J R, CHAO K, LU H J. Investigation of ignition transient in large segmented SRM[J]. Journal of Solid Rocket Technology, 2017, 40(2): 141-145. (in Chinese). doi: 10.7673/j.issn.1006-2793.2017.02.002
[5]	寇志海, 王清印, 李广超, 等. 航空发动机高温壁面热电偶测温技术应用[J]. 热能动力工程,2023,38(1):202-210. KOU ZH H, WANG Q Y, LI G CH, et al. Thermocouple measurement technology for high temperature wall in aero-engine[J]. Journal of Engineering for Thermal Energy and Power, 2023, 38(1): 202-210. (in Chinese).
[6]	WRBANEK J D, FRALICK G C. Thin film physical sensor instrumentation research and development at nasa glenn research center[C]. Proceedings of the 52nd International Instrumentation Symposium, 2006: 82-91. (查阅网上资料, 未找到本条文献出版者信息, 请确认) .
[7]	SOBCZYK J. Experimental study of the flow field disturbance in the vicinity of single sensor hot-wire anemometer[J]. EPJ Web of Conferences, 2018, 180: 02094. doi: 10.1051/epjconf/201818002094
[8]	苏铁, 陈爽, 杨富荣, 等. 双色平面激光诱导荧光瞬态燃烧场测温实验[J]. 红外与激光工程,2014,43(6):1750-1754. doi: 10.3969/j.issn.1007-2276.2014.06.010 SU T, CHEN SH, YANG F R, et al. Investigation of temperature of transient combustion using two-line PLIF[J]. Infrared and Laser Engineering, 2014, 43(6): 1750-1754. (in Chinese). doi: 10.3969/j.issn.1007-2276.2014.06.010
[9]	PAUL P H, NAJM H N. Planar laser-induced fluorescence imaging of flame heat release rate[J]. Symposium (International) on Combustion, 1998, 27(1): 43-50. doi: 10.1016/S0082-0784(98)80388-3
[10]	ZHOU B, KIEFER J, ZETTERBERG J, et al. Strategy for PLIF single-shot HCO imaging in turbulent methane/air flames[J]. Combustion and Flame, 2014, 161(6): 1566-1574. doi: 10.1016/j.combustflame.2013.11.019
[11]	李红, 李博, 高强, 等. OH/CH₂O基于PLIF测量得到的火焰面密度比较研究[J]. 燃烧科学与技术,2018,24(6):523-527. LI H, LI B, GAO Q, et al. Plane laser-induced fluorescence for flame surface density calculation of OH/CH₂O: A comparative study[J]. Journal of Combustion Science and Technology, 2018, 24(6): 523-527. (in Chinese).
[12]	RASMUSSEN C C, DHANUKA S K, DRISCOLL J F. Visualization of flameholding mechanisms in a supersonic combustor using PLIF[J]. Proceedings of the Combustion Institute, 2007, 31(2): 2505-2512. doi: 10.1016/j.proci.2006.08.007
[13]	KARIUKI J, DOWLUT A, YUAN R, et al. Heat release imaging in turbulent premixed methane–air flames close to blow-off[J]. Proceedings of the Combustion Institute, 2015, 35(2): 1443-1450. doi: 10.1016/j.proci.2014.05.144
[14]	FIALA T, SATTELMAYER T. Heat release and UV–Vis radiation in non-premixed hydrogen–oxygen flames[J]. Experiments in Fluids, 2015, 56(7): 144. doi: 10.1007/s00348-015-2013-8
[15]	CIARDIELLO R, PATHANIA R S, HELOU I E, et al. Lean blow-off investigation in a linear multi-burner combustor operated in premixed and non-premixed modes[J]. Applications in Energy and Combustion Science, 2022, 9: 100041. doi: 10.1016/j.jaecs.2021.100041
[16]	KARIUKI J, DOWLUT A, BALACHANDRAN R, et al. Heat release imaging in turbulent premixed ethylene-air flames near blow-off[J]. Flow, Turbulence and Combustion, 2016, 96(4): 1039-1051. doi: 10.1007/s10494-016-9720-y
[17]	MULLA I A, DOWLUT A, HUSSAIN T, et al. Heat release rate estimation in laminar premixed flames using laser-induced fluorescence of CH₂O and H-atom[J]. Combustion and Flame, 2016, 165: 373-383. doi: 10.1016/j.combustflame.2015.12.023
[18]	STRAKEY P A, WOODRUFF S D, WILLIAMS T C, et al. OH-PLIF measurements of high-pressure, hydrogen augmented premixed flames in the simval combustor[C]. 45th AIAA Aerospace Sciences Meeting and Exhibit, AIAA, 2007: 11867-11880.
[19]	MILLER J D, ENGEL S R, TROGER J W, et al. Characterization of a CH planar laser-induced fluorescence imaging system using a kHz-rate multimode-pumped optical parametric oscillator[J]. Applied Optics, 2012, 51(14): 2589-2600. doi: 10.1364/AO.51.002589
[20]	BOHON M D, GUIBERTI T F, ROBERTS W L. PLIF measurements of non-thermal NO concentrations in alcohol and alkane premixed flames[J]. Combustion and Flame, 2018, 194: 363-375. doi: 10.1016/j.combustflame.2018.05.024
[21]	SCHULZ C, SICK V, HEINZE J, et al. Laser-induced-fluorescence detection of nitric oxide in high-pressure flames with A-X(0, 2) excitation[J]. Applied Optics, 1997, 36(15): 3227-3232. doi: 10.1364/AO.36.003227
[22]	PALMER J L, MCMILLIN B K, HANSON R K. Multi-line fluorescence imaging of the rotational temperature field in a shock-tunnel free jet[J]. Applied Physics B, 1996, 63(2): 167-178. doi: 10.1007/BF01095269
[23]	HEINZE J, MEIER U, BEHRENDT T, et al. PLIF thermometry based on measurements of absolute concentrations of the OH radical[J]. Zeitschrift für Physikalische Chemie, 2011, 225(11-12): 1315-1341.
[24]	于欣, 杨超博, 彭江波, 等. 基于紫外可调谐激光吸收光谱技术的甲烷/空气平面预混火焰温度测量研究[J]. 光谱学与光谱分析,2016,36(4):1027-1032. YU X, YANG CH B, PENG J B, et al. Temperature measurement of CH₄/air premix flat flame based on the absorption spectroscopy technology of UV tunable laser[J]. Spectroscopy and Spectral Analysis, 2016, 36(4): 1027-1032. (in Chinese).
[25]	GRISCH F, ORAIN M. Role of planar laser-induced fluorescence in combustion research[J]. Journal of Aerospace Lab, 2009(1): 1-14.
[26]	YIP B, MILLE M F, LOZANO A, et al. A combined OH/acetone planar laser-induced fluorescence imaging technique for visualizing combusting flows[J]. Experiments in Fluids, 1994, 17(5): 330-336. doi: 10.1007/BF01874413
[27]	SEITZMAN J M, MILLER M F, ISLAND T C, et al. Double-pulse imaging using simultaneous OH/acetone PLIF for studying the evolution of high-speed, reacting mixing layers[J]. Symposium (International) on Combustion, 1994, 25(1): 1743-1750. doi: 10.1016/S0082-0784(06)80823-4
[28]	BRESSON A, BOUCHARDY P, MAGRE P, et al. OH/acetone PLIF and CARS thermometry in a supersonic reactive layer[C]. 10th AIAA/NAL-NASDA-ISAS International Space Planes and Hypersonic Systems and Technologies Conference, AIAA, 2001: 1759.
[29]	ELBAZ A M, ROBERTS W L. Experimental study of the inverse diffusion flame using high repetition rate OH/acetone PLIF and PIV[J]. Fuel, 2016, 165: 447-461. doi: 10.1016/j.fuel.2015.10.096
[30]	RANKIN B A, FUGGER C A, RICHARDSON D R, et al. Evaluation of mixing processes in a non-premixed rotating detonation engine using acetone PLIF[C]. 54th AIAA Aerospace Sciences Meeting, AIAA, 2016: 1198.
[31]	严浩, 张少华, 余西龙, 等. OH与CH₂O双组分平面激光诱导荧光对旋流燃烧室火焰结构与脉动特征的研究[J]. 航空动力学报,2019,34(4):894-907. YAN H, ZHANG SH H, YU X L, et al. Flame structure and dynamics characters inVestigation by OH and CH₂O planar laser-induced fluorescence in the swirl combustor[J]. Journal of Aerospace Power, 2019, 34(4): 894-907. (in Chinese).
[32]	陈晓丽, 金川, 苏秋成, 等. 基于激光诱导荧光法的同轴射流火焰中羟基自由基、甲醛、发热率与一氧化氮的二维可视化测量[J]. 分析测试技术与仪器,2021,27(3):182-188. CHEN X L, JIN CH, SU Q CH, et al. Two-dimensional visualization measurement of hydroxyl radical, formaldehyde, heat release rate and nitric oxide in co-flow jet flame based on planar laser induced fluorescence technology[J]. Analysis and Testing Technology and Instruments, 2021, 27(3): 182-188. (in Chinese).
[33]	梁剑寒, 李韵, 孙明波, 等. 超声速燃烧火焰放热区结构CH-PLIF成像技术[J]. 国防科技大学学报,2019,41(1):27-33. doi: 10.11887/j.cn.201901005 LIANG J H, LI Y, SUN M B, et al. CH-PLIF imaging of flame heat-release structures in supersonic combustion[J]. Journal of National University of Defense Technology, 2019, 41(1): 27-33. (in Chinese). doi: 10.11887/j.cn.201901005
[34]	吴戈, 李韵, 万明罡, 等. 平面激光诱导荧光技术在超声速燃烧火焰结构可视化中的应用[J]. 实验流体力学,2020,34(3):70-77. doi: 10.11729/syltlx20190168 WU G, LI Y, WAN M G, et al. Visualization of flame structure in supersonic combustion by planar laser induced fluorescence technique[J]. Journal of Experiments in Fluid Mechanics, 2020, 34(3): 70-77. (in Chinese). doi: 10.11729/syltlx20190168
[35]	关小伟, 刘晶儒, 黄梅生, 等. PLIF法定量测量甲烷-空气火焰二维温度场分布[J]. 强激光与粒子束,2005,17(2):173-176. GUAN X W, LIU J R, HUANG M SH, et al. Two-dimensional temperature field measurement in a methane-air flame by PLIF[J]. High Power Laser and Particle Beams, 2005, 17(2): 173-176. (in Chinese).
[36]	曹春丽, 徐胜利, 刘二伟. 双波长NO-PLIF法测量运动激波前后温度场的实验研究[J]. 中国科学技术大学学报,2012,42(12):977-983. doi: 10.3969/j.issn.0253-2778.2012.12.005 CAO CH L, XU SH L, LIU E W. Temperature measurement on moving shock wave by two-wavelength NO-PLIF method[J]. Journal of University of Science and Technology of China, 2012, 42(12): 977-983. (in Chinese). doi: 10.3969/j.issn.0253-2778.2012.12.005
[37]	宋东先, 谢辉, 邹庆武, 等. 单线双示踪粒子PLIF测温技术的开发[J]. 小型内燃机与车辆技术,2015,44(4):1-5,55. doi: 10.3969/j.issn.1671-0630.2015.04.001 SONG D X, XIE H, ZOU Q W, et al. The development of single-line two tracers PLIF temperature measurement technology in an optical engine[J]. Small Internal Combustion Engine and Vehicle Technique, 2015, 44(4): 1-5,55. (in Chinese). doi: 10.3969/j.issn.1671-0630.2015.04.001
[38]	梁帅, 张周, 丁海春, 等. 用PLIF测量GDI发动机滚流平面的混合气浓度[J]. 内燃机学报,2018,36(6):481-490. LIANG SH, ZHANG ZH, DING H CH, et al. Mixture distribution measurement in the tumble plane of a GDI engine via PLIF method[J]. Transactions of CSICE, 2018, 36(6): 481-490. (in Chinese).
[39]	任晓光, 王兰红, 董全, 等. 基于PLIF技术的天然气喷射流场摩尔浓度特性[J]. 内燃机学报,2020,38(5):417-425. REN X G, WANG L H, DONG Q, et al. Concentration characteristics in the flow field of a natural gas injection based on PLIF[J]. Transactions of CSICE, 2020, 38(5): 417-425. (in Chinese).
[40]	SCHMIDT J B, JIANG N, GANGULY B N. Nitric oxide PLIF measurement in a point-to-plane pulsed discharge in vitiated air of a propane/air flame[J]. Plasma Sources Science and Technology, 2014, 23(6): 065005. doi: 10.1088/0963-0252/23/6/065005
[41]	余响林, 王世敏, 许祖勋, 等. 光电功能性有机染料及其应用研究进展[J]. 染料与染色,2004,41(2):63-66,80. YU X L, WANG SH M, XU Z X, et al. Progress on the study of photoelectrical functional organic dyes and their applications[J]. Dyestuffs and Coloration, 2004, 41(2): 63-66,80. (in Chinese).
[42]	李海鹏, 韩奎, 沈晓鹏, 等. 半花菁衍生物分子第一超极化率频率色散效应的理论研究[J]. 光学学报,2005,25(5):655-660. doi: 10.3321/j.issn:0253-2239.2005.05.018 LI H P, HAN K, SHEN X P, et al. Theoretical studies on frequency-dispersion effect of first hyperpolarizabilities of hemicyanine derivatives[J]. Acta Optica Sinica, 2005, 25(5): 655-660. (in Chinese). doi: 10.3321/j.issn:0253-2239.2005.05.018
[43]	KITTLER C, DREIZLE A. Cinematographic imaging of hydroxyl radicals in turbulent flames by planar laser-induced fluorescence up to 5 kHz repetition rate[J]. Applied Physics B, 2007, 89(2): 163-166.
[44]	BOXX I, HEEGER C, GORDON R, et al. Simultaneous three-component PIV/OH-PLIF measurements of a turbulent lifted, C₃H₈-Argon jet diffusion flame at 1.5kHz repetition rate[J]. Proceedings of the Combustion Institute, 2009, 32(1): 905-912. doi: 10.1016/j.proci.2008.06.023
[45]	BOXX I, STÖHR M, CARTER C, et al. Sustained multi-kHz flamefront and 3-component velocity-field measurements for the study of turbulent flames[J]. Applied Physics B, 2009, 95(1): 23-29. doi: 10.1007/s00340-009-3420-4
[46]	BOXX I, ARNDT C M, CARTER C D, et al. High-speed laser diagnostics for the study of flame dynamics in a lean premixed gas turbine model combustor[J]. Experiments in Fluids, 2012, 52(3): 555-567. doi: 10.1007/s00348-010-1022-x
[47]	HAMMACK S, CARTER C, WUENSCHE C, et al. Continuous hydroxyl radical planar laser imaging at 50 kHz repetition rate[J]. Applied Optics, 2014, 53(23): 5246-5251. doi: 10.1364/AO.53.005246
[48]	HAMMACK S D, CARTER C D, SKIBA A W, et al. 20 kHz CH₂O and OH PLIF with stereo PIV[J]. Optics Letters, 2018, 43(5): 1115-1118. doi: 10.1364/OL.43.001115
[49]	PAN R C, RETZER U, WERBLINSKI T, et al. Generation of high-energy, kilohertz-rate narrowband tunable ultraviolet pulses using a burst-mode dye laser system[J]. Optics Letters, 2018, 43(5): 1191-1194. doi: 10.1364/OL.43.001191
[50]	RETZER U, PAN R C, WERBLINSKI T, et al. Burst-mode OH/CH₂O planar laser-induced fluorescence imaging of the heat release zone in an unsteady flame[J]. Optics Express, 2018, 26(14): 18105-18114. doi: 10.1364/OE.26.018105
[51]	FUGGER C A, HSU P S, JIANG N B, et al. 10-kHz simultaneous dual-plane stereo-PIV and OH-PLIF imaging[J]. Applied Physics B, 2020, 126(10): 167. doi: 10.1007/s00340-020-07522-4
[52]	SJÖHOLM J, KRISTENSSON E, RICHTER M, et al. Ultra-high-speed pumping of an optical parametric oscillator (OPO) for high-speed laser-induced fluorescence measurements[J]. Measurement Science and Technology, 2009, 20(2): 025306. doi: 10.1088/0957-0233/20/2/025306
[53]	HALLS B R, HSU P S, JIANG N B, et al. kHz-rate four-dimensional fluorescence tomography using an ultraviolet-tunable narrowband burst-mode optical parametric oscillator[J]. Optica, 2017, 4(8): 897-902. doi: 10.1364/OPTICA.4.000897
[54]	LI Z M, ROSELL J, ALDÉN M, et al. Simultaneous burst imaging of dual species using planar laser-induced fluorescence at 50 kHz in turbulent premixed flames[J]. Applied Spectroscopy, 2017, 71(6): 1363-1367. doi: 10.1177/0003702816678866
[55]	WANG Z K, STAMATOGLOU P, LI Z M, et al. Ultra-high-speed PLIF imaging for simultaneous visualization of multiple species in turbulent flames[J]. Optics Express, 2017, 25(24): 30214-30228. doi: 10.1364/OE.25.030214
[56]	ROY S, JIANG N B, HSU P S, et al. Development of a three-legged, high-speed, burst-mode laser system for simultaneous measurements of velocity and scalars in reacting flows[J]. Optics Letters, 2018, 43(11): 2704-2707. doi: 10.1364/OL.43.002704
[57]	FELVER J, SLIPCHENKO M N, BRAUN E L, et al. High-energy laser pulses for extended duration megahertz-rate flow diagnostics[J]. Optics Letters, 2020, 45(16): 4583-4586. doi: 10.1364/OL.400831
[58]	HSU P S, SLIPCHENKO M N, JIANG N B, et al. Megahertz-rate OH planar laser-induced fluorescence imaging in a rotating detonation combustor[J]. Optics Letters, 2020, 45(20): 5776-5779. doi: 10.1364/OL.403199
[59]	JAIN A, PARAJULI P, WANG Y J, et al. Hydroxyl radical planar laser-induced fluorescence imaging in flames using frequency-tripled femtosecond laser pulses[J]. Optics Letters, 2020, 45(17): 4690-4693. doi: 10.1364/OL.400930
[60]	ZHANG ZH L, YANG A L, WANG J, et al. OH planar laser-induced fluorescence imaging system using a kilohertz-rate 283 nm UV Ti: sapphire laser[J]. Applied Optics, 2023, 62(8): 1915-1920. doi: 10.1364/AO.484749
[61]	叶景峰, 张振荣, 李国华, 等. 激光激励煤油荧光光谱实验研究[C]. 中国力学大会2011暨钱学森诞辰100周年纪念大会论文集, 中国力学学会, 2011: 1-5. YE J F, ZHANG ZH R, LI G H, et al. The experiment study of laser induced kerosene fluorescence[C]. Review of the Chinese Conference on Theoretical and Applied Mechanics-2001 in Memorial of Tsien-Shen's 100th Anniversary, The Chinese Society of Theoretical and Applied Mechanics, 2011: 1-5. (in Chinese) (查阅网上资料, 未找到本条文献英文翻译, 请确认) .