• Acta Physica Sinica
  • Vol. 69, Issue 2, 029502-1 (2020)
Xing-Sheng Wang, Yan-Ming Ma, Xun Gao*, and Jing-Quan Lin*
DOI: 10.7498/aps.69.20190753 Cite this Article
Xing-Sheng Wang, Yan-Ming Ma, Xun Gao, Jing-Quan Lin. Near infrared characteristics of air plasma induced by nanosecond laser[J]. Acta Physica Sinica, 2020, 69(2): 029502-1 Copy Citation Text show less
Experiment setup for the near infrared emissions from ns laser-induced air plasma.纳秒激光诱导空气等离子体近红外辐射实验装置
Fig. 1. Experiment setup for the near infrared emissions from ns laser-induced air plasma.纳秒激光诱导空气等离子体近红外辐射实验装置
IR emissions of laser-induced air plasma varied with laser energy after 15 μs delay time.不同能量下激光诱导空气等离子体在激光作用15 μs后测到的红外辐射光谱
Fig. 2. IR emissions of laser-induced air plasma varied with laser energy after 15 μs delay time.不同能量下激光诱导空气等离子体在激光作用15 μs后测到的红外辐射光谱
IR emissions of laser-induced air and N2 plasma under 80 kPa.80 kPa气压下激光诱导空气和氮气等离子体红外辐射光谱
Fig. 3. IR emissions of laser-induced air and N2 plasma under 80 kPa. 80 kPa气压下激光诱导空气和氮气等离子体红外辐射光谱
IR emissions of laser-induced plasma of mixed gas with different pressure.O2和N2气体不同压强比的激光诱导等离子体红外辐射光谱
Fig. 4. IR emissions of laser-induced plasma of mixed gas with different pressure.O2和N2气体不同压强比的激光诱导等离子体红外辐射光谱
The fitting result of binary linear regression analysis.二元线性回归分析结果
Fig. 5. The fitting result of binary linear regression analysis.二元线性回归分析结果
Speciesλ/nm Aki/s–1Lower stateUpper state
Term symbolJTerm symbolJ
O I1128.63172.32 × 1072s22p3(4S0)3p 3P 12s22p3(4S0)3d 32
O I1128.64061.29 × 1072s22p3(4S0)3p 3P 12s22p3(4S0)3d 31
O I1128.69143.09 × 1072s22p3(4S0)3p 3P 22s22p3(4S0)3d 33
O I1128.70297.74 × 1062s22p3(4S0)3p 3P 22s22p3(4S0)3d 32
O I1128.73181.72 × 1072s22p3(4S0)3p 3P 02s22p3(4S0)3d 31
O I1129.51035.34 × 1062s22p3(4S0)3p 5P 12s22p3(4S0)4s 52
O I1129.76828.90 × 1062s22p3(4S0)3p 5P 22s22p3(4S0)4s 52
O I1130.23781.25 × 1072s22p3(4S0)3p 5P 32s22p3(4S0)3d 52
N I1129.1671.20 × 1072s22p2(3P)3p 47/22s22p2(3P)4s 4P 5/2
N I1131.3891.00 × 1072s22p2(3P)3p 45/22s22p2(3P)4s 4P 3/2
N I1132.3188.19 × 1062s22p2(3P)3p 43/22s22p2(3P)4s 4P 1/2
N I1246.12531.82 × 1072s22p2(3P)3p 23/22s22p2(3P)3d 2F 5/2
N I1246.96152.18 × 1072s22p2(3P)3p 25/22s22p2(3P)3d 2F 7/2
N I1358.13235.76 × 1062s22p2(3P)3 s 2P 3/22s22p2(3P)3p 21/2
N I1358.77106.31 × 1062s22p2(3P)3p 25/22s22p2(3P)4s 2P 3/2
N I1360.2271.07 × 1072s22p2(3P)3p 21/22s22p2(3P)3d 2D 3/2
N I1362.4181.33 × 1072s22p2(3P)3p 23/22s22p2(3P)3d 2D 5/2
N I1475.70731.06 × 1062s22p44P 5/22s22p2(3P)3p 47/2
N I1558.22876.5 × 1062s22p2(3P)3p 23/22s22p2(3P)4s 2P 3/2
Table 1. Identification of the observed emission lines of NI and OI
气体气压/kPa预测值实验值相对误差/%
Air801698421669031.76
701486121531362.95
601273821403179.21
501061511176739.79
4084921885164.06
30636915657512.56
20424602796451.80
Table 2. Comparison between predicted value and experimental value of the intensity of 1128 nm.
Xing-Sheng Wang, Yan-Ming Ma, Xun Gao, Jing-Quan Lin. Near infrared characteristics of air plasma induced by nanosecond laser[J]. Acta Physica Sinica, 2020, 69(2): 029502-1
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