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The presence of high- Zimpurities in magnetically confined fusion devices has different influences on the confinement property of the plasma due to the high cooling rate of high- Zimpurities. The first wall of EAST is equipped with molybdenum tiles, molybdenum particles sputtered from inevitable plasma-wall interaction enter into the plasma and become high- Zimpurity. In this paper, four fast-time-response extreme ultraviolet (EUV) spectrometers, a system which is upgraded in the EAST 2021 campaign, are used to monitor the line emission from impurity ions in the 5–500 Å wavelength range simultaneously. The in-situ wavelength calibration is carried out accurately using several well-known emission lines of low- and medium-Z impurity ions. The observed spectral lines are carefully identified based on the National Institute of Standards Technology (NIST) database, previously published experimental data and the time evolution of the normalized line intensity of emission lines from impurity ions. At the lower electron temperature ( T e0= 1.5 keV), the EUV spectra emitted from molybdenum ions in the range of 5–485 Å are systematically identified in EAST discharges accompanied with spontaneous sputtering events. As a result, two unresolved transition arrays of molybdenum spectra composed of Mo 19+-Mo 24+(Mo XX-Mo XXV) and Mo 16+-Mo 29+(Mo XVII-Mo XXX) are observed in the ranges of 15–30 Å and 65–95 Å. In addition, several spectral lines of lower molybdenum ions of Mo 4+-Mo 17+(Mo V-Mo XVIII) in the ranges of 27–60 Å and 120–485 Å are observed and identified on EAST for the first time, including a few strong and isolated forbidden and resonant lines, e.g. Mo XII at 329.414 Å, 336.639 Å and 381.125 Å, Mo XIII at 340.909 Å and 352.994 Å, Mo XIV at 373.647 Å and 423.576 Å, Mo XV at 50.448 Å, 57.927 Å and 58.832 Å. Six spectral lines are newly observed in the range of 27–32 Å, i.e. (27.21 ± 0.01) Å, (27.37 ± 0.01) Å, (28.99 ± 0.01) Å, (30.81 ± 0.01) Å, (31.54 ± 0.01) Å and (31.83 ± 0.01) Å, which may be Mo XV-Mo XVIII spectral lines. As a result, twelve strong and isolated spectral lines are chosen in routine observation for impurity transport physical study. The identification of these spectral lines not only enriches the molybdenum atom database, but also provides a solid experimental data base for magnetically confined devices to study the behavior and transport in core and edge plasmas of high-Z impurity.
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谱线 离子 电离能/eV 波长/Å 跃迁能级 实验值 参考值 Mo V Mo4+ 54.42 258.09 ± 0.03 258.069 4p54d33→ 4p64d21D2 324.98 ± 0.02 324.979 4p64d5f3H°4→ 4p64d23F4 327.13 ± 0.01 327.167 4p54d33→ 4p64d23P2 Mo VI Mo5+ 68.83 227.75 ± 0.04 227.801 4p5(2P°)4d(3F)5s2F°5/2→4p64d2D5/2 229.20 ± 0.04 229.262 4p66f2F°5/2→4p64d2D3/2 Mo VII Mo6+ 125.64 151.85 ± 0.04 151.747 4s24p5(2P°3/2)5d2[1/2] °1→ 4s24p61S0 235.66 ± 0.05 235.694 4s24p5(2P°3/2)5f2[3/2]1→ 4s24p5(2P°1/2)4d2[3/2]°2 Mo VIII Mo7+ 143.6 133.18 ± 0.03 133.168 4s24p4(3P)5d2P3/2→4s24p52P°3/2 134.34 ± 0.03 134.362 4s24p4(3P)5d4F5/2→4s24p52P°3/2 136.83 ± 0.03 136.782 4s24p4(3P)5d2D3/2→4s24p52P°3/2 Mo IX Mo8+ 164.12 132.03 ± 0.03 132.077 4s24p3(2P°)5d3P°1→4s24p41S0 158.53 ± 0.03 158.641 4s24p3(2P°1/2)5s (1/2, 1/2)°1→4s24p43P2 176.67 ± 0.04 176.682 4s24p3(2D°3/2)5s (3/2, 1/2)°2→4s24p41D2 231.90 ± 0.05 231.991 4s24p3(2D°)4d1F°3→4s24p4 1D2 237.76 ± 0.05 237.843 4s24p3(2D°)4d1D°2→4s24p4 1D2 Mo X Mo9+ 186.3 152.54 ± 0.04 152.683 4s24p2(3P)5s4P3/2→4s24p34S°3/2 157.65 ± 0.04 157.624 4s24p2(3P)5s2P3/2→4s24p32D°5/2 159.07 ± 0.04 159.049 4s24p2(3P)5s4P5/2→4s24p32D°5/2 159.42 ± 0.04 159.219 4s24p2(3P)5s4P3/2→4s24p32D°3/2 231.07 ± 0.04 231.110 4s24p2(1D)4d2F7/2→4s24p32D°5/2 239.03 ± 0.06 239.017 4s24p2(1S)4d2D5/2→4s24p32P°3/2 243.05 ± 0.06 243.071 4s24p2(1D)4d2D3/2→4s24p32D°5/2 Mo XI Mo10+ 209.3 146.65 ± 0.04 146.641 4s24p (2P°1/2)5s (1/2, 1/2)°1→4s24p23P2 322.12 ± 0.04 322.158 4s4p31P°1→ 4s24p21D2 Mo XII Mo11+ 230.28 131.37 ± 0.03 131.394 4s25s2S1/2→4s24p2P°1/2 250.09 ± 0.06 250.112 4s24d2D5/2→4s24p2P°3/2 329.53 ± 0.01 329.414 4s4p22P3/2→4s24p2P°3/2 336.51 ± 0.01 336.639 4s4p22P1/2→4s24p2P°3/2 381.13 ± 0.06 381.125 4s4p22D3/2→4s24p2P°1/2 Mo XIII Mo12+ 279.1 53.56 ± 0.02 53.551 3d94s24p3D°1→3d104s21S0 54.12 ± 0.02 54.101 3d94s24p1P°1→3d104s21S0 340.88 ± 0.01 340.909 3d104s4p1P°1→3d104s21S0 352.87 ± 0.03 352.994 3d104p23P1→3d104s4p3P°0 Mo XIV Mo13+ 302.6 51.98 ± 0.02 52.000 3d9(2D)4p2(3P)2P1/2→3d104p2P°3/2 52.77 ± 0.02 52.753 3d9(2D)4s4p (3P°)2P°3/2→3d104s2S1/2 121.68 ± 0.02 121.647 3d105s2S1/2→3d104p2P°3/2 241.78 ± 0.06 241.609 3d104d2D3/2→3d104p2P°1/2 373.55 ± 0.05 373.647 3d104p2P°3/2→3d104s2S1/2 423.57 ± 0.07 423.576 3d104p2P°1/2→3d104s2S1/2 Mo XV Mo14+ 544 29.48 ± 0.01 29.458 3d95f1P°1→3d10 1S0 29.81 ± 0.01 29.774 3d95f3D°1→3d10 1S0 35.39 ± 0.01 35.368 3d94f1P°1→3d10 1S0 50.43 ± 0.02 50.448 3d9(2D5/2)4p (5/2, 3/2)°1→3d101S0 58.04 ± 0.04 57.927 3d9(2D3/2)4s (3/2, 1/2)2→3d101S0 58.86 ± 0.04 58.832 3d9(2D5/2)4s (5/2, 1/2)2→3d101S0 347.47 ± 0.05 347.339 3d9(2D5/2)4p (5/2, 3/2)°3→3d9(2D5/2)4s (5/2, 1/2)3 365.77 ± 0.04 365.924 3d9(2D5/2)4p (5/2, 3/2)4→3d9(2D5/2)4s (5/2, 1/2)3 Mo XVI Mo15+ 591 32.92 ± 0.05 32.916 3p63d8(1G4)4f2[1]°3/2→3p63d92D5/2 34.03 ± 0.01 33.992 3p63d8(3F2)4f2[1]°3/2→3p63d92D3/2 54.46 ± 0.03 54.348 3p63d8(3F4)4s (4, 1/2)9/2→3p63d92D5/2 Mo XVIII Mo17+ 702 38.81 ± 0.01 38.700a 3d64p→3d7 a数据来源于文献[18], 其他数据来源于NIST数据库[25], 粗体表示可用于杂质诊断的谱线. -
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