Line Tables

These tables give observed air wavelengths for the 2000-20000 Å range for spectra other than Fr I. Outside of the 2000-20000 Å range, the wavelengths are vacuum wavelengths. Lines of Fr I are extrapolated vacuum wavelengths from known energy levels. All observed lines are from NIST ASD. All energy level information is from NIST ASD. Wavelengths from MIT Wavelength Tables have been omitted as this publication appears to still be under copyright. However, in some cases, the exact same wavelength is given by NIST and MIT; in that case, the line is included.

Line intensities have been adjusted in the visible region to match photographed visible spectra. Line intensities of Rn have been adjusted to match the Grotrian diagram of Rn I. Line intensities in the infrared and ultraviolet are less reliable, but every effort was made to estimate them as accurately as possible. The elements He, O, Cl, Ar, Kr, and Xe have had their NIR lines photographed out to roughly 11000 Å. The intensities of the "brightest" several IR lines of each of these elements, in the 7000-10000 Å range, can be trusted. For the range of 3800-8000 Å, estimated visual brightnesses (EVB) are given. A dash in either of the intensity columns means the line intensity would be less than one relative to other lines of the same spectrum.

All Spectra

H   He
Li Be   B C N O F Ne
Na Mg   Al Si P S Cl Ar
K Ca   Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr
Rb Sr   Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe
Cs Ba La Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb Lu Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn
Fr Ra Ac Th Pa U Np Pu Am Cm Bk Cf Es Fm Md No Lr Rf Db Sg Bh Hs Mt Ds Rg Cn Nh Fl Mc Lv Ts Og

Entire Range | 2000-10000 Å | Visible Region | Si CCD/CMOS Region | Thermal IR | Vacuum UV
Specific Wavelength (rounded):  Å  nm
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λ, Å E. Sp.# Rel.Int. EVB Lower Config Lower Term+J Lower Level Upper Config Upper Term+J Upper Level
3363.45 Ni II 435 -
3365.77 Ni I 285 - 3d9.(2D).4s 1D2 3409.937 3d8.(3F).4s.4p.(3P°) 33 33112.334
3366.17 Ni I 285 - 3d8.(3F).4s2 3F3 1332.164 3d9.(2D).4p 13 31031.02
3366.81 Ni I 55 -
3367.89 Ni I 55 - 3d9.(2D).4s 3D3 204.787 3d9.(2D).4p 32 29888.477
3369.57 Ni I 2500 - 3d8.(3F).4s2 3F4 0 3d9.(2D).4p °3 29668.918
3371.99 Ni I 345 - 3d8.(3F).4s2 3F3 1332.164 3d8.(3F).4s.4p.(3P°) 34 30979.749
3374.22 Ni I 225 - 3d9.(2D).4s 3D3 204.787 3d8.(3F).4s.4p.(3P°) 53 29832.779
3374.64 Ni I 105 -
3378.155 Ni II 1 - 3p6.3d9 2D5/2 0 3p6.3d8.(3P).4s 2P1/2 29593.46
3378.97 Ni II 435 -
3380.57 Ni I 3000 - 3d9.(2D).4s 1D2 3409.937 3d9.(2D).4p 11 32982.26
3380.74 Ni V 1 - 3d6 5D4 0 3d6 3F23 29570.8
3380.85 Ni I 210 - 3d8.(3F).4s2 3F2 2216.55 3d8.(3F).4s.4p.(3P°) 33 31786.162
3391.05 Ni I 1000 - 3d8.(3F).4s2 3F4 0 3d9.(2D).4p 34 29480.989
3392.99 Ni I 3000 - 3d9.(2D).4s 3D3 204.787 3d9.(2D).4p °3 29668.918
3401.05 Ni II 420 -
3409.58 Ni I 105 - 3d8.(3F).4s2 3F4 0 3d9.(2D).4p 33 29320.762
3413.48 Ni I 270 - 3d8.(3F).4s2 3F3 1332.164 3d9.(2D).4p 32 30619.414
3413.94 Ni I 270 - 3d9.(2D).4s 3D2 879.816 3d8.(3F).4s.4p.(3P°) 52 30163.124
3414.3 Ni VII 1 - 3d4 5D4 2392 3d4 3H4 31672
3414.76 Ni I 1000 - 3d9.(2D).4s 3D3 204.787 3d9.(2D).4p 34 29480.989
3417.2 Ni XVII 1 - 3s.3p 30 264431 3s.3p 32 293686
3420.737 Ni I 1 - 3d8.(3F).4s2 3F2 2216.55 3d9.(2D).4p 12 31441.635
3423.71 Ni I 1500 - 3d9.(2D).4s 3D1 1713.087 3d9.(2D).4p 31 30912.817
3432.65 Ni V 1 - 3d6 5D4 0 3d6 3F24 29123.7
3433.56 Ni I 2000 - 3d9.(2D).4s 3D3 204.787 3d9.(2D).4p 33 29320.762
3437.28 Ni I 840 - 3d8.(3F).4s2 3F4 0 3d8.(3F).4s.4p.(3P°) 54 29084.456
3438.877 Ni II 1 - 3p6.3d9 2D5/2 0 3p6.3d8.(3P).4s 2P3/2 29070.93
3446.16 Ni V 1 - 3d6 5D3 889.7 3d6 3F22 29899.2
3446.26 Ni I 4000 - 3d9.(2D).4s 3D2 879.816 3d9.(2D).4p 32 29888.477
3452.89 Ni I 1000 - 3d9.(2D).4s 3D2 879.816 3d8.(3F).4s.4p.(3P°) 53 29832.779
3458.47 Ni I 4500 - 3d9.(2D).4s 3D1 1713.087 3d9.(2D).4p 32 30619.414
3461.65 Ni I 4500 - 3d9.(2D).4s 3D3 204.787 3d8.(3F).4s.4p.(3P°) 54 29084.456
3467.5 Ni I 180 - 3d8.(3F).4s2 3F3 1332.164 3d8.(3F).4s.4p.(3P°) 52 30163.124
3469.49 Ni I 210 - 3d8.(3F).4s2 3F2 2216.55 3d9.(2D).4p 13 31031.02
3472.54 Ni I 1500 - 3d9.(2D).4s 3D2 879.816 3d9.(2D).4p °3 29668.918
3483.77 Ni I 510 - 3d8.(3F).4s2 3F2 2216.55 3d9.(2D).4p 31 30912.817
3485.62 Ni V 1 - 3d6 5D3 889.7 3d6 3F23 29570.8
3485.89 Ni I 120 - 3d9.(2D).4s 3D1 1713.087 3d8.(3F).4s.4p.(3P°) 51 30392.003
3492.96 Ni I 1000 - 3d9.(2D).4s 3D2 879.816 3d9.(2D).4p 31 29500.674
3498.192 Ni I 1 - 3d8.(3F).4s2 3F4 0 3d8.(3F).4s.4p.(3P°) 53 28578.018
3500.85 Ni I 630 - 3d8.(3F).4s2 3F3 1332.164 3d9.(2D).4p 32 29888.477
3502.6 Ni I 65 - 3d8.(3F).4s2 3F4 0 3d8.(3F).4s.4p.(3P°) 55 28542.105
3507.69 Ni I 55 - 3d8.(3F).4s2 3F3 1332.164 3d8.(3F).4s.4p.(3P°) 53 29832.779
3510.34 Ni I 2500 - 3d9.(2D).4s 3D1 1713.087 3d9.(2D).4p 30 30192.251
3513.93 Ni I 255 - 3d9.(2D).4s 3D1 1713.087 3d8.(3F).4s.4p.(3P°) 52 30163.124
3515.05 Ni I 1000 - 3d9.(2D).4s 3D2 879.816 3d9.(2D).4p 33 29320.762
3518.97 Ni V 1 - 3d6 5D2 1489.9 3d6 3F22 29899.2
3519.77 Ni I 645 - 3d8.(3F).4s2 3F2 2216.55 3d9.(2D).4p 32 30619.414
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