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
6657.92 Xe I 15 3 5p5.(2P°3/2).6p 2[3/2]2 79212.465 5p5.(2P°3/2).8d 2[1/2]°1 94228.004
6658.118 Co II 45 9 3d7.(4F).5p 56 95998.735 3d7.(4F).5d 5F5 111013.838
6658.213 V II - - 3d3.(4F).4d 3G4 75615.399 3d3.(4F7/2).4f 2[9/2]°5 90630.288
6658.36 Dy I 65 13
6658.552 Sc II 1500 267 3p6.3d.4d 3G5 60457.12 3p6.3d.4f 35 75471.25
6658.639 Tm I 150 31 4f12.(3H5).5d3/2.6s2 (5,3/2)9/2 24348.692 4f13.(2F°7/2).6s.6d.(1D) 1[11/2]°11/2 39362.651
6658.999 Sc II 240 49 3p6.3d.4d 3G5 60457.12 3p6.3d.4f 34 75470.24
6659.05 Pm II 4000 798
6659.36 W I 20 4
6659.4 Hf I 15 3
6659.496 Th II - - 6d3 2F7/2 22834.13401 6d2.(3P).7p °5/2 37846.1686
6659.674 Mo I 15 3 4d5.(4D).5s b 5D4 20157.802 4d4.5s.(6D).5p z 54 35169.407
6660. Mn XII 15 3 3s2.3p2 3P0 0 3s2.3p2 3P2 15010
6660.2 Pb II 1000 206 6s2.7s 2S1/2 59448.56 6s2.7p 21/2 74458.99
6660.223 V II - - 3d3.(4F).4d 3G3 75422.913 3d3.(4F5/2).4f 2[7/2]°4 90433.288
6660.52 Si II 600 119 3s.3p.(3P°).4s 43/2 116978.38 3s.3p.(3P°).4p 4D5/2 131988.05
6660.676 Ar I 80 16 3s2.3p5.(2P°3/2).4p 2[3/2]1 106087.2598 3s2.3p5.(2P°1/2).6s 2[1/2]°0 121096.605
6660.74 V II 2 - 3d3.(4F).4d 3H5 75346.305 3d3.(4F5/2).4f 2[11/2]°6 90355.515
6660.84 Nb I 225 44
6660.961 Cu II 10 2 3d9.4p 32 73353.2957 3d8.4s2 3P2 88362.001
6661.0744 Cr I 405 81 3d4.(5D).4s.4p.(3P°) z 54 33816.0334 3d4.4s.5s f 5D4 48824.4834
6661.1 Sn II 8 2 5s2.6d 2D5/2 90351.894 5s2.6f 27/2 105360.3
6661.105 I I 50 10 5s2.5p4.(3P2).6p 2[2]°5/2 64906.29 5s2.5p4.(3P2).9s 2[2]5/2 79914.682
6661.25 Pm II 1000 199
6661.324 Ni I 1 - 3d8.(3F).4s.4p.(3P°) 32 34163.264 3d9.(2D5/2).4d 2[3/2]1 49171.151
6661.4 La I 240 48 5d2.(3F).6s 4F9/2 4121.572 5d2.(3F).6p 49/2 19129.31
6661.64 Dy I 80 16
6661.67 Cl II 585 118
6661.68 Pm I 5000 997
6661.81 Os I 15 3
6662.24 Ta I 15 3 5d4.(3H).6s a 4H9/2 21153.33 5d3.6s.(3H).6p z 4H°?7/2 36159.13
6662.2685 Th I 225 44 6d3.(4F).7s 5F3 7502.287636 6d2.7s.7p 52 22508.04658
6662.389 V I 30 6 3d4.(3F2).4s b 4F5/2 15688.862 3d3.(2G).4s.4p.(3P°) y 47/2 30694.344
6662.5 Mg IV 15 3 2s2.2p4.(1D).3s 2D3/2 582578.4 2s2.2p4.(3P).3p 41/2 597583.6
6662.52 Ho I 585 117
6662.6321 Th II 3 1 6d3 2H9/2 15305.26434 5f.(2F°).6d2.(1G) °11/2 24309.22275
6662.7 Si III 20 4 3s.6f 32 242410.88 3s.9d 3D1 257415.6
6662.733 C I 135 26 2s2.2p.3p 3P1 71364.93596 2s2.2p.6s 32 86369.622
6662.9 Si III 20 4 3s.6f 33 242411.27 3s.9d 3D3 257415.6
6663.044 C I 270 54 2s2.2p.3p 3P2 71385.40992 2s2.2p.5d 32 86389.425
6663.1 Si III 20 4 3s.6f 34 242411.7 3s.9d 3D3 257415.6
6663.1 Xe II 2 - 5p4.(1D2).6p 2[2]°3/2 131923.79 5p4.(3P1).6d 2[3]5/2 146927.86
6663.14 Ru I 585 118 4d7.(a 4F).5p z 54 28014.79 4d7.(a 4F).6s e 5F4 43018.57
6663.18 W I 15 3
6663.2321 Fe I 8 2 3d6.(5D).4s.4p.(1P°) y 53 36766.966 3d6.(5D).4s (4D).5s g 5D3 51770.557
6663.25 Cm I 10000 1995
6663.4417 Fe I 55 11 3d6.4s2 a 3P21 19552.478 3d6.(5D).4s.4p.(3P°) z 30 34555.597
6663.61 W I 15 3
6663.6969 Th I 10 2 6d2.7s2 1G4 8111.004545 5f.6d2.7s 54 23113.54761
6663.76 Pm I 4000 798
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