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
5194.586 Ge I 15 12 4s2.4p.5s 31 37702.3054 4s2.4p.6p 3P2 56947.7693
5195.219 Ge II 45 40 4s2.5d 2D5/2 100130.812 4s2.7f 27/2 119373.92
5205.6488 Ge II 135 117 4s2.4f 27/2 100317.283 4s2.7g 2G9/2 119521.837
5205.8371 Ge II 100 88 4s2.4f 25/2 100317.976 4s2.7g 2G7/2 119521.835
5229.37 Ge III 45 40
5256.61 Ge III 40 37
5265.892 Ge I 95 87 4s2.4p.5s 31 37702.3054 4s2.4p.6p 3P1 56687.1584
5513.264 Ge I 105 105 4s2.4p.5s 32 39117.9021 4s2.4p.6p 1D2 57250.9427
5522.989 Ge II 270 263 4s2.6p 23/2 101244.635 4s2.8d 2D5/2 119345.75
5564.742 Ge I 135 141 4s2.4p.5s 32 39117.9021 4s2.4p.6p 3S1 57083.2021
5607.012 Ge I 150 142 4s2.4p.5s 32 39117.9021 4s2.4p.6p 3P2 56947.7693
5616.137 Ge I 105 107 4s2.4p.5s 31 37702.3054 4s2.4p.6p 3P0 55503.2026
5621.428 Ge I 120 125 4s2.4p.5s 30 37451.6893 4s2.4p.6p 1P1 55235.8344
5655.962 Ge I 150 142 4s2.4p.5s 32 39117.9021 4s2.4p.6p 3D3 56793.46
5664.227 Ge I 105 107 4s2.4p.5s 11 40020.5604 4s2.4p.6p 1S0 57670.326
5664.844 Ge I 90 89 4s2.4p.5s 32 39117.9021 4s2.4p.(2P°1/2).4f 2[7/2]3 56765.748
5691.958 Ge I 165 160 4s2.4p.5s 31 37702.3054 4s2.4p.6p 3D2 55266.0902
5701.778 Ge I 105 106 4s2.4p.5s 31 37702.3054 4s2.4p.6p 1P1 55235.8344
5717.878 Ge I 90 88 4s2.4p.5s 30 37451.6893 4s2.4p.6p 3D1 54935.8479
5801.032 Ge I 70 64 4s2.4p.5s 31 37702.3054 4s2.4p.6p 3D1 54935.8479
5802.093 Ge I 105 95 4s2.4p.5s 11 40020.5604 4s2.4p.6p 1D2 57250.9427
5893.3886 Ge II 2000 1870 4s2.5s 2S1/2 62403.028 4s2.5p 23/2 79366.494
6021.0414 Ge II 1000 795 4s2.5s 2S1/2 62403.028 4s2.5p 21/2 79006.853
6078.394 Ge II 225 157 4s.4p.(3P°).5s 45/2 124732.4 4s.4p.(3P°).5p 4D7/2 141179.7
6267.141 Ge II 50 27 4s2.5d 2D3/2 100089.97 4s2.6f 25/2 116041.81
6268.066 Ge II 150 81 4s2.4f 27/2 100317.283 4s2.6g 2G9/2 116266.75
6268.344 Ge II 105 54 4s2.4f 25/2 100317.976 4s2.6g 2G7/2 116266.75
6283.4519 Ge II 105 52 4s2.5d 2D5/2 100130.812 4s2.6f 27/2 116041.231
6336.3766 Ge II 75 36 4s2.5p 21/2 79006.853 4s2.6s 2S1/2 94784.381
6484.1812 Ge II 315 107 4s2.5p 23/2 79366.494 4s2.6s 2S1/2 94784.381
6557.488 Ge I 135 35 4s2.4p.5s 11 40020.5604 4s2.4p.6p 3D2 55266.0902
6780.51 Ge II 690 91 4s2.6p 23/2 101244.635 4s2.7d 2D5/2 115988.77
6966.3209 Ge II 300 19 4s.4p2 2D3/2 65015.672 4s2.5p 23/2 79366.494
7049.3694 Ge II 930 39 4s.4p2 2D5/2 65184.738 4s2.5p 23/2 79366.494
7130.117 Ge I 135 4 4s2.4p.5p 3D3 48104.1003 4s2.4p.7d (3/2,5/2)°4 62125.233
7145.3899 Ge II 645 16 4s.4p2 2D3/2 65015.672 4s2.5p 21/2 79006.853
7330.38 Ge I 150 1 4s2.4p.5p 1P1 46765.2705 4s2.4p.7d (1/2,3/2)°2 60403.365
7353.332 Ge I 105 1 4s2.4p.5p 3D2 46834.3798 4s2.4p.7d (1/2,5/2)°3 60429.908
7384.208 Ge I 150 1 4s2.4p.5p 3D1 45985.592 4s2.4p.8s (1/2,1/2)°1 59524.276
7402.645 Ge I 135 1 4s2.4p.5p 1P1 46765.2705 4s2.4p.6d (3/2,3/2)°2 60270.231
7511.57 Ge I 150 - 4s2.4p.5s 31 37702.3054 4s2.4p.5p 1S0 51011.4392
7776.2 Ge I 10 - 4s2.4p.5p 3D2 46834.3798 4s2.4p.6d (1/2,5/2)°2 59690.604
7833.573 Ge I 20 - 4s2.4p.5p 3D1 45985.592 4s2.4p.6d (1/2,3/2)°2 58747.644
7837.632 Ge I 15 - 4s2.4p.5p 3D1 45985.592 4s2.4p.6d (1/2,3/2)°1 58741.04
7853.77 Ge I 10 - 4s2.4p.5p 1P1 46765.2705 4s2.4p.8s (1/2,1/2)°0 59494.515
7878.12 Ge I 15 - 4s2.4p.5p 3D2 46834.3798 4s2.4p.8s (1/2,1/2)°1 59524.276
7962.265 Ge I 10 - 4s2.4p.4d 12 48480.048 4s2.4p.(2P°3/2).5f 2[5/2]3 61035.83
7983.327 Ge I 10 - 4s2.4p.4d 12 48480.048 4s2.4p.(2P°3/2).5f 2[7/2]3 61002.709
8031.037 Ge I 20 - 4s2.4p.5p 3D3 48104.1003 4s2.4p.6d (3/2,5/2)°4 60552.366
8044.162 Ge I 10 - 4s2.4p.5p 3P1 48088.3504 4s2.4p.7d (1/2,5/2)°2 60516.308
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