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利用YAG激光(波长1.06μm,脉宽为10 ns)烧蚀Al靶产生的三条Al Ⅲ等离子体谱线(452.92 nm,451.25 nm,415.01 nm),在局部热力学平衡近似下,利用玻尔兹曼图,测定了等离子体电子温度在不同激光能量下的变化特性。随着激光能量的增加,电子温度从14800 K近似单调的上升到20000 K,随后反而有所下降。在电子温度达最高时,连续辐射谱强度并未达最大值。同时还观测到,Al的原子谱线和离子谱线强度随激光能量有不同的变化特点。利用玻尔兹曼图的最小二乘方拟合,测得Al Ⅲ谱线447.99 nm(4f2F7/2-5g2G9/2)跃迁的几率约为(10.4士0.8)×108s-1。

The temperature of laser-produced Al plasmas (LPP) have been measured at different laser energy by using the model of local thermodynamic equilibrium (LTE). The electron temperature changed from 14800 K to 20000 K when the laser energy increased from 30 mJ/pulse to 45 mJ/pulse, then , the temperature had some decrease along the laser energy increasing. The intensities of Al Ⅰ spectra lines have shown similar variant property, but differetnt from other Al ions spectra lines. Meanwhile, the transition probability of 447.99 nm line of Al Ⅲ was measured by the Boltzmann plots was about (9~10)× 108 s-1.

参考文献

[1] Ready J F . Effects of High-power Laser Radiation [M]. New York: Academic, 1971.
[2] Key M N. Spectroscopy of laser-produced plasmas [J]. Adv. Atomic. Molec. Phys., 1980, 16:201~280
[3] Colon C. Measurement of the Stark broadening and shift parameters for several ultraviolet lines of singly ionized aluminium [J]. J. Appl. Phys., 1993, 73(10): 4752~4758
[4] 张树东,陈冠英等.激光诱导Al等离子体时间分辨光谱[J].应用激光,待发表
[5] Thorne A P. Spectrophysics [M]. Chanman and Hall
[6] 张树东,陈冠英等.Al激光诱导等离子体光谱Stark加宽观测[J].原子与分子物理学报,1999,16(4):475~461
[7] 张树东,陈冠英等.激光诱导Al等离子体温度的测定及时间变化特性研究[J].西北师范大学学报,2000,36(2):22~26
[8] Wiese W L. Atomic Transition Probabilities [M]. Vol Ⅱ, 1969, Washington D C
[9] Victor Kaufman. Wavelengths and energy-level classifications for the spectra of Aluminium [J]. J. Phys. Chem. Ref. Data, 1991, 20(5): 775~808
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