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
7462.414 Fe II 25 - 3d6.(3D).4s b 4D5/2 31387.9788 3d6.(5D).4p z 45/2 44784.7859
7462.62 Si III 90 - 3s.4d 3D2 201598.28 3s.5p 31 214994.65
7463.08 La I 40 - 5d2.(3F).6s 2F7/2 8052.162 5d2.(3F).6p °7/2 17910.17
7463.2313 Fe II - - 3d6.(5D).5p w 63/2 91843.485 3d6.(3P2).4d 2D5/2 105238.815
7463.382 Fe I - - 3d6.(5D).4s.4p.(1P°) x 53 40842.154 3d7.(4F).4d e 5H4 54237.213
7463.427 Th I - - 5f.6d2.7s 35 22399.39666 6d4 3F14 35794.3768
7463.85 Sc I 10 - 3d.4s.(1D).4p 27/2 21085.829 3d.4s.(3D).5s 4D5/2 34479.99
7463.86 Hf I 150 1
7464. Ga I 15 - 4s2.5p 23/2 33155.07 4s2.9d 2D5/2 46549
7464.36 Gd I 330 1
7464.367 Ni I 2 - 3d8.(3F).4s2 3F2 2216.55 3d8.(3P).4s2 3P2 15609.844
7464.871 Sc II 5 - 3p6.3d.5p 32 66459.64 3p6.3d.5d 3F2 79852.02
7465.01 Kr I - - 4s2.4p5.(2P°3/2).4d 2[7/2]°4 97797.287 4s2.4p5.(2P°3/2).8f 2[9/2]5 111189.5
7465.35 Si III 15 - 3s.4d 3D1 201597.73 3s.5p 32 214989.27
7465.45 C I 25 - 2s.2p3 31 75254.0017 2s2.2p.(2P°3/2).7f 2[3/2]2 88645.36
7465.6258 Fe II - - 3d5.(4G).4s.4p.(1P°) 47/2 108906.631 3d6.(3H).6s 4H7/2 122297.664
7465.65 Si III 15 - 3s.4d 3D2 201598.28 3s.5p 32 214989.27
7465.7789 Fe II - - 3d6.(5D).5p w 63/2 91843.485 3d6.(3P2).4d 4P5/2 105234.246
7466.32 Si III 95 - 3s.4d 3D3 201599.48 3s.5p 32 214989.27
7466.4 C I 30 - 2s.2p3 30 75256.1696 2s2.2p.(2P°3/2).7f 2[3/2]1 88645.37
7466.519 Fe I - - 3d7.(4F).4p y 32 38678.039 3d6.(5D).4s (6D).4d e 5P2 52067.469
7466.771 Fe II - - 3d6.(5D).5p 41/2 91199.776 3d6.(5D).5d 6D3/2 104588.729
7467.24 Ne II 70 - 2s2.2p4.(3P).5s 2P1/2 304440.2089 2s2.2p4.(1D).4p 21/2 317828.313
7467.75 Ta I 210 1 5d4.(5D).6s a 6D3/2 9975.81 5d3.6s.(5F).6p z 45/2 23363.09
7467.99 Kr II - - 4s2.4p4.(3P).5d 4F5/2 165075.6 4s2.4p4.(3P2).5f 2[3]°7/2 178462.5
7468.31 N I 4 - 2s2.2p2.(3P).3s 4P5/2 83364.62 2s2.2p2.(3P).3p 43/2 96750.84
7468.75 Te II 765 3
7468.91 Ru I 840 3 4d7.(a 4F).5p z 52 30958.8 4d7.(a 4F).6s e 5F1 44343.91
7468.9381 Fe II - - 3d6.(5D).5p 45/2 90638.823 3d6.(5D).5d 4F5/2 104023.921
7468.987 I I 390 1 5s2.5p4.(3P2).6p 2[3]°7/2 65669.988 5s2.5p4.(3P2).7d 2[4]9/2 79054.985
7469.0565 Th I 2 - 5f.6d.7s2 34 14206.91694 6d4 3H5 27591.80212
7469.191 Fe I - - 3d6.(3P2).4s.4p.(3P°) w 53 43922.668 3d6.4s.(6D).5d 7F4 57307.32
7469.938 Ti I 45 - 3d3.(4F).4s a 5F4 6742.756 3d2.(3F).4s.4p.(3P°) z 33 20126.062
7470.09 C I 30 - 2s.2p3 32 75255.29373 2s2.2p.(2P°3/2).7f 2[5/2]3 88638.32
7470.4146 Fe II - - 3d6.(5D).5p 67/2 90300.628 3d6.(5D).5d 4F9/2 103683.078
7470.53 Eu I 25 - 4f7.(8S°).5d (9D°).6s a 83/2 15137.72 4f7.(8S°).5d (9D°).6p z 10F3/2 28519.97
7470.76 Sm I 165 1
7470.89 Rn I 15 -
7471.164 Ar I 2 - 3s2.3p5.(2P°3/2).4s 2[3/2]°1 93750.5978 3s2.3p5.(2P°1/2).4p 2[3/2]1 107131.7086
7471.35 Co II 4 - 3d7.(4F).5s e 5F4 84586.868 3d7.(4F).5p 33 97967.697
7471.41 Al II 30 - 3s.3d 1D2 110089.83 3s.4f 13 123470.5
7471.581 Mn II 4 - 3d4.4s2 c 5D2 55116.333 3d5.(4P).4p y 51 68496.694
7471.7285 Fe II - - 3d6.(3H).5p 411/2 108483.877 3d6.(3H).6s 4H13/2 121863.975
7471.862 Fe II - - 3d6.(5D).5p 43/2 91208.892 3d6.(5D).5d 6D3/2 104588.729
7471.89 Pa I 3000 11
7472. Xe II 2 - 5p4.(1D2).6p 2[2]°5/2 132207.76 5p4.(3P1).6d 2[3]7/2 145587.61
7472.01 Xe I 70 - 5p5.(2P°3/2).5d 2[1/2]°1 79986.618 5p5.(2P°3/2).5f 2[3/2]2 93366.245
7472.4383 Ne I 65 - 2s2.2p5.(2P°3/2).3p 2[1/2]1 148257.7898 2s2.2p5.(2P°3/2).3d 2[3/2]°1 161636.6175
7472.751 Fe I - - 3d6.(5D).4s (6D).5s e 7D4 43163.326 3d6.4s.(6D).6p 74 56541.596
7473.1841 V I 4 - 3d4.(5D).4s a 6D7/2 2311.369 3d4.(3F2).4s b 4F5/2 15688.862
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