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
7578.73 Re I 465 1
7578.909 S II 60 - 3s2.3p2.(1D).3d 2G9/2 127128.35 3s2.3p2.(1D).4p 27/2 140319.23
7578.98 Ga II 1 - 4s.5p 11 120550.431 4s.6s 1S0 133741.2
7579. Ti XVI 10 - 2s.(2S).2p4.(3P) 4P3/2 620470 2s.(2S).2p4.(3P) 4P1/2 633660
7579.023 Cu II 30 - 3d9.(2D3/2).5s 2[3/2]2 110366.1542 3d9.(2D3/2).5p 2[3/2]°2 123556.8261
7579.08089 Fr I - - 7p 23/2 13923.998 9p 21/2 27118.21
7579.26 Tc 100 -
7579.77 Bk I 10000 17
7579.85 Cu II 10 - 3d9.(2D5/2).5s 2[5/2]2 108335.6078 3d8.(3F).4s.4p.(3P°) 13 121524.8509
7580.1951 Fe II - - 3d6.(5D).5p 43/2 92225.549 3d6.(3F2).4d 4G5/2 105414.186
7580.265 Ti I 120 - 3d3.(2P).4s b 3P0 17995.487 3d2.(3P).4s.4p.(3P°) v 31 31184.01
7580.6 Cr V 3 - 3p6.3d2 3F2 0 3p6.3d2 1D2 13188
7580.61 Tm I 70 - 4f13.(2F°5/2).6s.6p.(3P°2) (5/2,2)9/2 28024.01 4f13.(2F°7/2).6s.8s.(3S1) (7/2,1)°7/2 41211.943
7580.764 Mg II 25 - 2p6.5f 27/2 103689.92 2p6.10g 2G9/2 116877.54
7581. S VI - - 2p6.6p 23/2 583674.1 2p6.6d 2D5/2 596861.3
7581.0918 Fe II - - 3d5.(4D).4s.4p.(3P°) 65/2 92018.727 3d6.(5D).5d 6G5/2 105205.808
7581.11 Ca II 60 -
7581.6511 Fe II - - 3d6.(3P1).4p 45/2 92274.123 3d6.(3F2).4d 4D3/2 105460.233
7582.1214 Fe I - - 3d6.(5D).4s.4p.(1P°) x 53 39969.853 3d7.(4F).4d h 5D4 53155.145
7582.35 Sc I 10 -
7582.514 Co II 35 - 3d7.(4F).5p 51 97153.739 3d7.(4F).6s 5F1 110338.346
7583.21 Nb I 15 -
7583.273 Cu II - - 3d9.(2D5/2).4d 2[1/2]0 116576.5758 3d8.(1D).4s.4p.(3P°) 31 129759.75
7583.4 Se I 210 -
7583.7754 Cs I - - 5p6.5d 2D3/2 14499.2568 5p6.9p 23/2 27681.6782
7583.7877 Fe I 6 - 3d6.4s2 b 3G3 24338.767 3d7.(4F).4p y 32 37521.161
7583.91 Eu I 375 1 4f7.(8S°).6s.6p.(3P°) z 10P11/2 15581.58 4f7.(8S°).6s (9S°).7s e 109/2 28763.82
7584.01 Ti II 15 - 3d2.(3F).4d f 4F7/2 68952.1302 3d2.(3F).4f 47/2 82134.1565
7584.29 Xe I 7 - 5p5.(2P°3/2).5d 2[7/2]°4 80196.629 5p5.(2P°3/2).5f 2[9/2]4 93378.199
7584.48 Sc I 25 - 3d2.(3F).4p 45/2 32696.808 3d2.(3F).4d 4H7/2 45878.05
7584.68 Xe I 135 - 5p5.(2P°3/2).5d 2[7/2]°4 80196.629 5p5.(2P°3/2).5f 2[9/2]5 93377.475
7584.705 Mg I 6 - 3s.3p 31 21870.464 3s.3p 11 35051.264
7585.79175 Th I 210 - 6d2.7s2 3P0 2558.056752 6d2.7s.7p 51 15736.968041
7585.8 S VI - - 2p6.6p 23/2 583674.1 2p6.6d 2D3/2 596853
7585.85 Sm II 80 -
7586.0182 Fe I 10 - 3d7.(4F).4p z 55 34782.421 3d7.(4F).5s e 3F4 47960.94
7586.6443 Fe II - - 3d6.(5D).5p 67/2 88853.535 3d6.(5D).6s 6D7/2 102030.965
7587.4136 Kr I 180 - 4s2.4p5.(2P°3/2).5s 2[3/2]°1 80916.768 4s2.4p5.(2P°3/2).5p 2[1/2]0 94092.8626
7587.6241 Fe II - - 3d6.(5D).5p 45/2 90638.823 3d6.(5D).5d 4F7/2 103814.552
7587.7853 Fe II - - 3d6.(3H).5s e 4H7/2 98568.907 3d6.(3F2).5p 27/2 111744.362
7588.2 Gd I 15 -
7588.2104 Cr II 15 - 3d3.(4P).4s.4p.(3P°) x 67/2 94452.6258 3d4.(5D).5d 6D7/2 107627.3409
7588.3048 Fe I - - 3d6.(5D).4s.4p.(1P°) x 54 40594.432 3d7.(4F).4d f 5G4 53768.979
7588.31 Sm II 55 -
7588.4648 Zn II 270 - 3d10.5s 2S1/2 88437.15 3d10.5p 23/2 101611.4
7588.48 P I 10 - 3s2.3p2.(3P).4p 45/2 66544.243 3s2.3p2.(3P).5d 4D3/2 79718.49
7588.61 Ti II 10 - 3d2.(3F).4d f 4F3/2 68769.3365 3d2.(3F).4f 45/2 81943.4136
7588.64 Pr III 15 -
7589.2 Ho I 80 -
7589.3152 Ar II 210 - 3s2.3p4.(3P).3d 4P5/2 147875.9477 3s2.3p4.(3P).4p 43/2 161048.7411
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