巢湖学院学报 ›› 2019, Vol. 21 ›› Issue (6): 80-85.doi: 10.12152/j.issn.1672-2868.2019.06.012

• 数理科学 • 上一篇    下一篇

实验参数对激光诱导Cu等离子体特性的影响

1.傅院霞:(1) 蚌埠学院理学院;(2)安徽师范大学光电材料科学与技术安徽省重点实验室 2.徐丽、 肖伟: 蚌埠学院理学院
  

  1. 蚌埠学院理学院
  • 收稿日期:2019-08-29 出版日期:2019-11-25 发布日期:2020-03-13
  • 通讯作者: 傅院霞(1981-)女,安徽潜山人,蚌埠学院理学院讲师,主要从事激光光谱和团簇的理论和实验研究.
  • 作者简介:傅院霞(1981-)女,安徽潜山人,蚌埠学院理学院讲师,主要从事激光光谱和团簇的理论和实验研究.
  • 基金资助:
    国家自然科学基金项目(项目编号:11604003);安徽省高等学校自然科学研究重点项目(项目编号:KJ2019A0857);光电材料科学与技术安徽省重点实验室项目(项目编号:OMST201703)

Effects of Experimental Parameters on Properties of Laser-induced Cu Plasma

1.FU Yuan-xia:(1) Department of Science, Bengbu University;(2)Anhui Province Key Laboratory of#br# Optoelectronic Materials Science and Technology, Anhui Normal University 2. XU Li,XIAO Wei: Department of Science, Bengbu University   

  1. Department of Science, Bengbu University
  • Received:2019-08-29 Online:2019-11-25 Published:2020-03-13
  • Contact: FU Yuan-xia:1. Department of Science, Bengbu University, Bengbu Anhui 233030; 2. Anhui Province Key Laboratory of Optoelectronic Materials Science and Technology, Anhui Normal University, Wuhu Anhui 241000
  • About author:FU Yuan-xia:1. Department of Science, Bengbu University, Bengbu Anhui 233030; 2. Anhui Province Key Laboratory of Optoelectronic Materials Science and Technology, Anhui Normal University, Wuhu Anhui 241000

摘要: 实验主要研究样品温度(铜片)、ICCD 延迟对离子体特性的影响,通过波长为532 nm的激光聚焦到铜片,利用光接收器接收等离子体中原子和离子的发射光谱,从而处理得到光谱图和信噪比图像。结果显示门宽在110 ns到500 ns内,门宽越大,谱线强度以及信噪比越强,再考虑局部热平衡条件,所以门宽为200 ns 是最优;延迟在200 ns 到800 ns 内,可得600 ns 的延迟是最优;铜片温度在常温到110益内改变,铜片温度越高,信噪比越好,所以110益是最优参数。利用洛伦兹拟合求得谱线强度I 的值以及所选取谱线的半高全宽(FWHM)等,从而分别算出所选取的实验参数对应的的Cu 等离子体的电子温度以及电子密度,进而得到电子温度和电子密度随着样品温度、延迟的演化趋势。在样品铜片温度处于常温到110益范围内,Cu 等离子体电子温度从4752 K升至7231 K曰ICCD 延迟在200 ns至800 ns范围内,电子温度从14230 K降至1160 K。实验过程中选取了Cu的波长为465.2 nm 的谱线,并查阅出该谱线的电子碰撞系数计算得到电子密度。可得到铜片温度处于常温至110益时,铜等离子体的电子密度从2.041伊1017 cm-3升到2.732伊1017 cm-3曰ICCD 延迟处于200 ns至800 ns时,电子密度从3.51伊1017 cm-3下降至2.149伊1017 cm-3。

关键词: 激光诱导Cu 等离子体, 电子温度, 电子密度, 样品温度

Abstract: The sample temperature (copper), ICCD delay influence on laser induced Cu plasma characteristics were studied. Through the wavelength of 532nm emitting laser focus on the copper, using the optical receiver accept atoms and ions in the plasma emission spectrum, then the spectrum and the signal to noise ratio were obtained. The results are shown as follows: Considering the local heat balance condition and the stronger spectral line and signal-to-noise ratio, from 110ns to 500ns, the optimal gate width is 500ns; from 200ns to 600ns, the optimal delay is 600ns; Copper temperature from room temperature to 110益, the higher the temperature of the copper, the better the signal-to-noise ratio, so that 110益is the optimal parameters. Lorentz fitting and gaussian fitting were used to obtain the intensity I value of the spectral line and the half-height and full width (FWHM) of the selected spectral line, so as to calculate the electron temperature and electron density of the Cu plasma corresponding to the selected experimental parameters, and then obtain the evolution trend diagram of the electron temperature and electron density with the sample temperature and delay. The copper temperature from 20益to 110益, the electron temperature from 4752K to 7231K;the delay ranges from 200ns to 800ns, and the electron temperature drops from 14230K to 1160K. During the experiment, a spectral line with a wavelength of 465.2nm of Cu was selected, and the electron collision coefficient of the spectral line was consulted to calculate the value of electron density. Then the copper temperature from 20 to 110, the electron density rose from 2.041 cm-3 to 2.732 cm-3;When the delay of ICCD between 200ns and 800ns,the electron density decreased from 3.51 cm-3 to 2.149 cm-3.

Key words: Laser induced Cu plasma, Electronic temperature, Electron density, The sample temperature

中图分类号: 

  • O657.3