|
|
|
|
|
|
Progress of Thomson Scattering Diagnostic on HL-2A Tokamak |
SHANG Jie1, 2, HUANG Yuan2, YANG Kai1, CHEN Bao-wei1, LIU Chun-hua2, YANG Yi1 |
1. China Institute for Radiation Protection, Taiyuan 030006, China
2. Southwestern Institute of Physics, Chengdu 610225, China |
|
|
Abstract The diagnosis of incoherent laser Thomson scattering only needs to assume that the electron velocity satisfies the Maxwell distribution, and the measured data of plasma electron temperature and electron density are accurate and reliable. It is an important diagnostic tool in the Tokamak and other magnetically confined fusion research device, and it is developing towards the measurement requirements of high reliability, high spatial resolution and high repetition rate, while high reliability is the premise condition. The Thomson scattering cross section of electron is very small, and its total cross section is σT=6.65×10-25 cm2. Generally, the Q-switched Nd∶YAG laser is used as the scattering light source. The laser pulse width is about 10 ns, and the pulse energy is about 3 J. The scattering spectrum is measured and analyzed by a 5~8 channel polychromator. One of the key problems of laser scattering diagnosis is how to collect the scattering-related electric pulse output from photoelectric detection module. In the past, charge-sensitive analogue-to-digital converters (Q-ADCs, such as CMC080 module) were used to integrate the scattered pulse signal on the sampling capacitor over a certain time width (such as 50 ns), so as to obtain the strength value of the scattered signal. This method is difficult to eliminate circuit noise and external interference. Now, fast digitizers (vertical resolution ≥10 bits, sampling frequency f≥1 GS·s-1, such as V1742B module) are used to collect the data in the time period including the scattering signal (such as 300~500 ns), so as to obtain the data sequence superimposed by the scattering pulse signal, the disturbance of plasma light and background noise. In this paper, the least square method is used to fit the scattering pulse with Gaussian function, and then the scattering pulse is numerically integrated into 50 ns-width to get the strength value of the scattering signal. The results show that the use of high-speed synchronous acquisition technology can eliminate most of the interference with digital filtering technology, so as to improve the signal-to-noise ratio, and its amplitude can reach about 10 times. After more accurate and reliable spectral data are extracted, the error-weighted least square method is used to process the data at the confidence level of 95%. A. C. Selden scattering spectral expression is used to estimate the parameters of electron temperature, and the measured value of electron temperature is obtained. The statistical error is about 3%, which is better than the previous 10%.
|
Received: 2020-01-22
Accepted: 2020-04-17
|
|
|
[1] Peacock N J, Robinson D C, Forrest M J, et al. Nature, 1969, 224: 488.
[2] Huang Y, Zhang P, Feng Z, et al. Review of Scientific Instruments, 2007, 78(11): 113501.
[3] Zang Q, Zhao J Y, Li Y, et al. Review of Scientific Instruments, 2011, 82(6): 063502.
[4] Walsh M J, Arends E R, Carolan P G, et al. Review of Scientific Instruments, 2003, 74(3): 1663.
[5] Kurzan B, Jakobi M, Murmann H. Plasma Phys. Control. Fusion, 2004, 46(1): 299.
[6] Carlstrom T N, Campbell G L, Deboo J C, et al. Review of Scientific Instruments, 1992, 63(10): 4901.
[7] Yamada I, Narihara K, Funaba H, et al. Review of Scientific Instruments, 2010, 81(10): 10D522.
[8] Van der Meiden H J, Barth C J, Oyevaar T, et al. Review of Scientific Instruments, 2004, 75(10): 3849.
[9] See www.caen.it for MOD. V1742, V1742x. MUTx/06.
[10] Minami T, Itoh Y, Yamada I, et al. Review of Scientific Instruments, 2014, 85: 11D837.
[11] Selden A C. Physics Letter A, 1980, 79(5): 405.
[12] Feng Z, Wang Y Q, Hou Z P, et al. Journal of Instrumentation, 2017, 12: C11012.
[13] SHANG Jie, HUANG Yuan, LIU Chun-hua, et al(商 洁, 黄 渊, 刘春华, 等). Laser & Optoelectronics Progress(激光与光电子学进展), 2015, 52(11): 111201.
[14] Press W H, Teukolsky S A, Vetterling W T, et al. Numerical Recipes in C. Second Edition.
[15] Huang Y, Wang Y Q, Hou Z P, et al. Review of Scientific Instruments, 2018, 89: 10C116.
[16] Huang Y, Wang Y Q, Hou Z P, et al. Journal of Instrumentation, 2019, 14: C11021.
[17] LIU Chun-hua, HOU Zhi-pei, WANG Yu-qin, et al(刘春华,侯智培,王瑜琴,等). High Power Laser and Particle Beams(强激光与粒子束), 2019, 31(2): 022003. |
[1] |
GUO Wei1, CHANG Hao2*, XU Can3, ZHOU Wei-jing2, YU Cheng-hao1, JI Gang2. Effect of Continuous Laser Irradiation on Scattering Spectrum
Characteristics of GaAs Cells[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2023, 43(12): 3674-3681. |
[2] |
JIANG Chun-xu1, 2, TAN Yong1*, XU Rong3, LIU De-long4, ZHU Rui-han1, QU Guan-nan1, WANG Gong-chang3, LÜ Zhong1, SHAO Ming5, CHENG Xiang-zheng5, ZHOU Jian-wei1, SHI Jing1, CAI Hong-xing1. Research on Inverse Recognition of Space Target Scattering Spectral
Image[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2023, 43(10): 3023-3030. |
[3] |
LI Chang-ming1, CHEN An-min2*, GAO Xun3*, JIN Ming-xing2. Spatially Resolved Laser-Induced Plasma Spectroscopy Under Different Sample Temperatures[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2023, 43(07): 2032-2036. |
[4] |
DENG Chen-yang, LIAO Ning-fang*, LI Ya-sheng, LI Yu-mei. Reconstruction of Spectral Bidirectional Reflectance Distribution Function for Metallic Coatings Based on Additivity of Scattering Spectrum[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2023, 43(07): 2043-2049. |
[5] |
LI Ru, YANG Xin, XING Qian-yun, ZHANG Yu. Emission Spectroscopy Study of Remote Ar Plasma[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2023, 43(02): 394-400. |
[6] |
SHI Jing1, 2, TAN Yong1, CHEN Gui-bo1, LI Shuang1, CAI Hong-xing1*. Inversion of Object Materials and Their Proportions Based on
Scattering Spectra[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2022, 42(08): 2340-2346. |
[7] |
GONG Zheng1, LIN Jing-jun2*, LIN Xiao-mei3*, HUANG Yu-tao1. Effect of Heating and Cooling on the Characteristic Lines of Al During Melting[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2022, 42(02): 598-602. |
[8] |
CHEN Chuan-jie1, 2, FAN Yong-sheng3, FANG Zhong-qing1, 2, WANG Yuan-yuan1, 2, KONG Wei-bin1, 2, ZHOU Feng1, 2*, WANG Ru-gang1, 2. Research on the Electron Temperature in Nanosecond Pulsed Argon Discharges Based on the Continuum Emission[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2021, 41(08): 2337-2342. |
[9] |
DONG Xiang-cheng1, CHEN Jian-hong2*, LIU Guang-qiao1. Characteristic Analysis of Continuous Radiation Spectrum of Lightning Plasma[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2021, 41(05): 1612-1616. |
[10] |
ZHOU Bing1, LIU Tian-shu2, MU Shuo2, WANG Peng-jie2, SHEN Qing-wu1, LUO Jie1, 2*. Using Spectroscopy Methods to Analyze the Key Textural Characteristics of Fermented Milk With High Creaminess Intensity[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2021, 41(04): 1194-1198. |
[11] |
DAI Li-juan1, DING Le-ming1, LI Wei-tao2, QIAN Zhi-yu2. Study on the Application of Scattering Spectrum With Small Source-Detector Separation in Pain Measurement[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2020, 40(12): 3743-3747. |
[12] |
LI Peng1, LI Zhi2, XU Can2, FANG Yu-qiang2. Research on the Scattering Spectrum of GaAs-Based Triple-Junction Solar Cell Based on Thin-Film Interference Theory[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2020, 40(10): 3092-3097. |
[13] |
WANG Li, FU Yuan-xia, XU Li,GONG Hao, RONG Chang-chun. The Effect of Sample Temperature on Characteristic Parameters of the Nanosecond Laser-Induced Cu Plasma[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2019, 39(04): 1247-1251. |
[14] |
FENG Cai-ping1, SUI Xiao-feng1, CHEN Chong2, GUO Hui-yuan2, WANG Peng-jie2*. Spectroscopic Analysis of Effect of Sodium Citrate on the Properties of Transglutaminase Goat’s Milk Gels[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2018, 38(08): 2505-2510. |
[15] |
XU Chen1, 2, HUA Xue-ming1, 2*, YE Ding-jian1, 2, MA Xiao-li1, 2, LI Fang1, 2, HUANG Ye1, 2. Study of the Effect of Interference during Multi-Wire GMAW Based on Spectral Diagnosis Technique[J]. SPECTROSCOPY AND SPECTRAL ANALYSIS, 2018, 38(07): 1993-1997. |
|
|
|
|