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
4020.25 Am I 105 1
4020.287 V I 15 - 3d4.(5D).4p z 67/2 24838.578 49705e 6D7/2 49705.393
4020.387 Sc I 450 7 3d.4s2 2D3/2 0 3d.4s.(3D).4p 23/2 24866.172
4020.483 Fe I 1 - 3d6.4s2 b 3D3 29371.812 3d6.(3G).4s.4p.(3P°) t 34 54237.415
4020.539 V I 3 - 3d4.(3D).4s b 4D5/2 20789.112 45654o 25/2 45654.368
4020.76 Tc 645 9
4020.882 Sr I 165 2 5s.4d 1D2 20149.685 5s.11f 13 45012.82
4020.8874 Fe II - - 3d6.(5D).5p 67/2 88853.535 3d6.(5D).6d 1137167/2 113716.636
4020.9 Co I 375 5 3p6.3d8.(3F).4s b 4F9/2 3482.82 3p6.3d7.(4F).4s.4p.(3P°) z 49/2 28345.86
4020.915 Th II - - 5f.(2F°).6d2.(3F) °9/2 17722.98541 5f2.6d+5f.6d.7p 9/2 49837.6587
4020.96 Pr II 195 3
4021.1078 Ti I 10 - 3d2.(3F).4s.4p.(3P°) z 53 16961.442 3d2.4s.(4F).4d e 5H3 41823.213
4021.341 Mn I 2 - 3d5.4s2 b 4D5/2 30419.61 3d5.(4D).4s.4p.(3P°) x 43/2 55279.91
4021.385 Cr I 15 - 3d5.(2I).4s a 3I7 31047.9572 3d4.(1I).4s.4p.(3P°) u 36 55907.998
4021.4 Cs XXXIV 1 - 3d4 5D2 139000 3d4 5D3 163860
4021.414 V I - - 3d4.(3D).4s b 4D5/2 20789.112 3d3.(2F).4s.4p.(3P°) p 43/2 45648.952
4021.58 In II 90 1 5s.4f 13 123699.17 5s1/2,F=5.11g 148557.89
4021.6 Xe III - - 5s2.5p3.(4S°).5d 31 121922.75 5s2.5p3.(4S°).6p 5P1 146781.48
4021.6025 Fe I 1 - 3d6.4s2 a 3P21 19552.478 3d6.(3P2).4s.4p.(3P°) w 51 44411.16
4021.682 V I 10 - 3d4.(5D).4p z 63/2 24648.114 49506e 6D1/2 49506.305
4021.725 Fe III - - 3d5.(b 2F).4s 3F4 93388.77 3d5.(4P).4p 53 118246.74
4021.8151 Ti I 585 8 3d2.(3F).4s.4p.(3P°) z 53 16961.442 3d2.4s.(4F).4d e 5G4 41818.8088
4021.866 Fe I 120 2 3d7.(2G).4s a 3G3 22249.429 3d6.(3H).4s.4p.(3P°) z 34 47106.484
4021.909 V I 8 - 3d4.(3P2).4s b 4P1/2 15078.387 3d4.(3F2).4p s 43/2 39935.176
4021.92 Tm III 50 1
4022.095 V I 15 - 3d3.4s2 a 4F5/2 137.383 3d4.(5D).4p y 67/2 24992.909
4022.0959 Th II 450 6 5f.7s2 25/2 4490.26167 5f2.(3F).7s 5/2 27593.9678
4022.115 C I 35 1 2s2.2p.3s 30 60333.4476 2s2.2p.5p 3P1 85188.967
4022.115 W I 120 2 5d4.6s.(6D).6p 71 20064.3 5d4.6s.(6D).7s 7D2 44919.84
4022.16 Ru I 270 4 4d6.5s2 a 5D3 8575.42 4d6.5s.(a 6D).5p y 53 33430.65
4022.17 In II 20 - 5s.4f 13 123699.17 5s1/2,F=4.11g 148554.36
4022.2124 Fe I - - 3d7.(4P).4s b 3P2 22838.323 3d6.(3G).4s.4p.(3P°) w 53 47693.239
4022.2597 Cr I 60 1 3d5.(4F).4s a 5F2 31355.1192 3d5.(4F).4p v 53 56209.743
4022.27 Ce II 30 - 4f2.(3F).6s 2F7/2 9053.629 4f2.(3F4).6p1/2 °9/2 33908.193
4022.326 Fe III - - 3d5.(b 2F).4s 3F3 93392.55 3d5.(4P).4p 53 118246.74
4022.33 Gd II 150 2
4022.42 Ne II - - 2s2.2p4.(3P).4p 23/2 294086.4608 2s2.2p4.(3P).7s 4P3/2 318940.046
4022.57 Cr I 2 - 3d5.(2I).4s a 3I5 31055.2777 3d4.(1I).4s.4p.(3P°) u 36 55907.998
4022.595 Tm I 65 1 4f13.(2F°).6s2 25/2 8771.243 4f12.(3F2).5d5/2.6s2 7/2 33623.78
4022.629 Cu I 50 1 3d10.4p 21/2 30535.324 3d10.5d 2D3/2 55387.667
4022.71 Pr II 55 1
4022.735 Fe I 2 - 3d7.(2D2).4s a 3D3 26224.969 3d6.(5D).4s (6D).5p t 54 51076.628
4022.76 Ho II 1000 18
4022.83 W I 40 1
4022.841 C I 55 1 2s2.2p.3s 31 60352.6584 2s2.2p.5p 3P2 85203.6756
4022.96 Re I 135 2
4023.05 V I 3 - 3d3.4s2 a 4P3/2 9637.039 3d3.(2D2).4s.4p.(3P°) 45/2 34486.787
4023.09 Ac II 20 -
4023.14 Gd I 210 3
4023.14 Rh I 60 1 4d8.(1D).5s b 2D3/2 14382.19 4d8.(1D).5p y 23/2 39231.38
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