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
3825.697 Nb IV 735 1 4d.6p 13 196387.02 4d.6d 3D3 222518.65
3825.7 Au I 45 -
3825.84 Bk II 10000 15
3825.874 V II - - 3d3.(2G).4p z 14 49723.6766 3d3.(4F).4d 3G5 75854.2212
3825.877 Nb IV 915 1 4d.6p 32 196388.25 4d.6d 3D3 222518.65
3825.8809 Fe I 540 1 3d7.(4F).4s a 5F4 7376.764 3d7.(4F).4p y 53 33507.123
3826.0214 Th II 2 - 5f.6d.(3F°).7s 49/2 12488.28836 5f.7s.(1F°).7p 9/2 38617.6823
3826.05 Gd II 30 -
3826.15 Kr II - - 4s2.4p4.(1D).5p 23/2 152190.13 4s2.4p4.(1D).5d 2D5/2 178318.69
3826.2 Sm II 135 -
3826.27 Xe II - - 5p4.(3P2).6p 2[3]°5/2 113512.36 5p4.(3P2).6d 2[1]3/2 139640.43
3826.373 Sr IV 8 - 4s2.4p4.(3P1).6p 2[1]°1/2 361194.32 4s2.4p4.(3P0).6d 2[2]3/2 387321.32
3826.386 Tm I 45 - 4f13.(2F°).6s2 27/2 0 4f13.(2F°5/2).6s.6p.(3P°1) (5/2,1)5/2 26126.907
3826.4142 Cr I 105 - 3d5.(4P).4s a 5P2 21847.8349 3d5.(4G).4p u 53 47974.5512
3826.434 V I 4 - 3d4.(3F2).4s a 2F7/2 19078.112 45204o 25/2 45204.697
3826.51 U II 960 1
3826.613 Mn I 4 - 3d5.(6S).4s.4p.(3P°) z 63/2 24779.32 3d5.4s.(7S).6s g 6S5/2 50904.68
3826.622 Sc IV 55 - 3s2.3p5.4d 11 453972.7 3s2.3p5.(2P°3/2).4f 2[5/2]2 480097.9
3826.626 Fe I - - 3d6.4s2 a 3H4 19788.251 3d6.(3F2).4s.4p.(3P°) x 53 45913.497
3826.63 Kr III - - 4s2.4p3.(2P°).5p 3P1 209284.41 4s2.4p3.(4S°).6d 51 235409.76
3826.657 Rb II 15 - 4p5.(2P°3/2).5p 2[3/2]2 158711.854 4p5.(2P°3/2).5d 2[3/2]°2 184836.897
3826.667 Tm I 45 - 4f12.(3H6).5d3/2.6s2 (6,3/2)9/2 13119.61 4f12.5d.6s.6p °9/2 34457.853
3826.67 Pr II 35 - 4f3.(4I°).5d 56 3893.46 4f3.(4I°).6p? 5H?7 30018.1
3826.68 Eu II 25 -
3826.693 Mo I 35 - 4d4.5s2 a 5D2 11454.362 4d4.5s.(6D).5p z 52 37579.174
3826.71 Cd II - - 4d9.5s2 2D5/2 69258.91 4d10.6p 23/2 95383.63
3826.7696 V I 40 - 3d4.(5D).4s a 4D1/2 8413.009 3d3.(4F).4s.4p.(1P°) v 43/2 34537.299
3826.8067 Ar II 7 - 3s2.3p4.(3P).4p 45/2 157673.4134 3s2.3p4.(3P).4d 4D5/2 183797.4473
3826.8412 Fe I 6 - 3d7.(2G).4s a 3G4 21999.13 3d6.(3G).4s.4p.(3P°) v 53 48122.928
3826.849 Ta I 135 - 5d3.6s2 a 4F5/2 2010.1 5d3.6s.(5F).6p y 45/2 28133.88
3826.86 Xe I 6 - 5p5.(2P°3/2).6s 2[3/2]°1 68045.156 5p5.(2P°3/2).9p 2[3/2]1 94168.86
3826.9209 Cu II 2 - 3d9.(2D5/2).5p 2[3/2]°2 120092.3828 3d9.(2D5/2).6d 2[1/2]1 146215.634
3826.9492 Th II 225 - 6d3 4P1/2 14349.3888 6d2.(3F).7p °3/2 40472.451
3826.9685 Ti I 135 - 3d3.(4F).4s b 3F2 11531.761 3d3.(2D2).4p u 32 37654.69
3826.9688 V II 85 - 3d3.(2D2).4s b 3D2 20617.0735 3d3.(4P).4p z 32 46740.01
3827.079 Fe II - - 3d6.(1D2).4s c 2D5/2 38164.22 3d6.(3F2).4p z 27/2 64286.354
3827.1102 Ti II 30 - 3d2.(1D).4p y 25/2 39476.9244 3d2.(3F).4d f 2F7/2 65598.8926
3827.154 Mo I 30 - 4d4.5s2 a 3F3 23668.079 4d5.(4F).5p u 33 49789.746
3827.187 Sr IV 10 - 4s2.4p4.(1D2).6p 2[3]°5/2 370570.27 4s2.4p4.(1D2).6d 2[4]7/2 396691.71
3827.307 Sc I 35 - 3d2.(3F).4s 2F7/2 15041.902 3d2.(3P).4p 25/2 41162.506
3827.33 Gd II 40 -
3827.41 Bk I 10000 15
3827.4684 Ti I 35 - 3d2.(3F).4s.4p.(3P°) z 53 16961.442 3d2.4s.(4F).4d g 5F2 43080.9622
3827.569 Ir II 210 - 5d7.(2D2).6s 3D3 26391.28 5d7.(4F5/2).6p (5/2,1/2)°2 52510.06
3827.57 Pu I 285 -
3827.5713 Fe I 4 - 3d7.(2G).4s a 3G5 21715.732 3d6.(3F2).4s.4p.(3P°) x 35 47834.55
3827.59 Cl II 50 -
3827.6362 Ti I 55 - 3d3.(2H).4s a 3H4 18037.213 3d2.4s.(4F).5p 33 44155.596
3827.717 Zr III 285 - 4d.4f 33 120794.02 4d.(2D3/2).5g 2[7/2]4 146911.81
3827.8224 Fe I 210 - 3d7.(4F).4s a 3F3 12560.934 3d7.(4F).4p y 32 38678.039
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