Abstract:Laser induced breakdown spectroscopy with long-pulse laser(500 μs) was used to generate plasma of soil sample in air. The spectroscopy emission characteristic of soil plasma was investigated under the low power-density conditions. Intense continuum background could not be detected (402~409 and 420~436 nm) and the long-pulse laser induced plasma had a longer overall life time (about 220~270 μs), which was different from the dynamic characteristics using nanosecond laser and ultra-short pulse laser. Besides, the spectral lines of Pb Ⅰ405.78 nm and Cr Ⅰ425.43 nm appeared at about 210 and 190 μs. Intensity of Pb Ⅰ405.78 nm and Cr Ⅰ425.43 nm increased as time passed by, reaching to its maximum at 320 and 350 μs, respectively. The study results showed that increased interaction time between laser and sample contributed to the formation of “quasi-stable state plasma”. The relative standard deviation was 2.21%~6.35% concluded by 8 times repeated experiments, which showed a better stability of soil plasma by using a long-pulse laser. The detection limits of Pb and Cr were 34.7 and 40.0 mg·kg-1, respectively, which was below the trace element thresholds for Class 1 soil used in the environmental quality standard in China. Parameters characterizing a laser-induced plasma were obtained with the temperature of 6612 K and electron density of 3.7×1017 cm-3 in the condition of long-pulse laser. Experimental results showed that it was in local thermodynamic equilibrium.
Key words:Long-pulse laser induced plasmas; Life-time of plasma; Relative standard deviation; Limit of detection
[1] Nunes L C, Braga J W B, Trevizan L C,et al. Journal of Analytical Atomic Spectrometry, 2010, 25: 1453.
[2] Pandhija S, Rai N K, Rai A K, et al. Applied Physics B, 2010, 98: 231.
[3] Gondal M A, DastageerA, MaslehuddinM, et al. Optics and Laser Technology, 2012, 3(44): 566.
[4] YU Ke-qiang, ZHAO Yan-ru, LIU Fei,et al(余克强, 赵艳茹, 刘 飞,等). Spectroscopy and Spectral Analysis(光谱学与光谱分析), 2016, 36(3): 827.
[5] Franois Brygo, Dutouquet C, Guern F L,et al. Applied Surface Science, 2006, 252: 2131.
[6] Eland K L, Stratis D N, Lai Tianshu,et al. Appl. Spectrosc., 2001, 55: 279.
[7] Eland K L, Stratis D N, Gold D M,et al. Appl. Spectrosc., 2001, 55: 286.
[8] ZHANG Shan-shan, DU Chuan-mei, FANG Xia,et al(章姗姗, 杜传梅, 方 霞,等). Journal of Atomic and Molecular Physics(原子与分子物理学报), 2008, 25(4): 911.
[9] FAN Jian-mei, YAO Guan-xin, ZHANG Xian-yi,et al(樊建梅, 姚关心, 张先燚,等). Chinese J. Lasers(中国激光), 2010, 37(8): 1956.
[10] CUI Zhi-feng, DU Chuan-mei, FANG Xia,et al(崔执凤, 杜传梅, 方 霞,等). Journal of Anhui Normal University·Natural Science(安徽师范大学学取·自然科学版), 2007, 30(3): 233.
[11] LI Ming(李 明). Theoretical and Experimental Studies on High Power Laser Induced Liquid Plasma. Nanjing: Nanjing University of Science and Technology, 2010. 19.
[12] XU Song-ning, JIANG Ran, NING Ri-bo,et al(徐送宁, 姜 冉, 宁日波,等). Chinese J. Lasers(中国激光), 2015, 42(11): 1115005.
[13] Guo L B, Hu W, Zhang B Y,et al. Optics Express, 2011, 19(15): 14067.
[14] SU Xue-jiao(苏雪娇). The Effects of Cavity Confinement on Laser-Induced Breakdown Spectroscopy. Jinhua: Zhejiang Normal University, 2015. 12.
[15] YE Tai-bing(叶太兵). Experimental Investigation on Laser Plasma Shielding. Nanjing: Nanjing University of Science and Technology, 2007. 15.
[16] XIN Ren-xuan(辛仁轩). Emission Spectral Analysis(等离子体发射光谱分析). Beijing: Chemical Industrial Press(北京: 化学工业出版社), 2004.
[17] NIST Atomic Spectra Database. http://physics.nist.gov/PhysRefData/ASD/lines_form.html
[18] Griem H R. Plasma Spectroscopy. New York: McGraw-Hill, 1964.