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
1728. Hg I 85 - 5d10.6s.6p 31 39412.237 5d9.6s2.(2D5/2).7s 2[5/2]2 97309.84
1731.823 Hg II 7 - 5d9.6s2 2D3/2 50555.567 5d10.7p 21/2 108298.183
1759.75 Hg III - -
1762. Hg I 270 - 5d10.6s.6p 31 39412.237 5d10.6p2 3P2 96190
1775.2 Hg I - - 5d10.6s.6p 30 37644.982 5d10.6p2 3P1 93980
1792.775 Hg II - -
1793.921 Hg II 25 - 5d9.6s2 2D3/2 50555.567 5d9.6s.6p (2D<3/2>,3P<2>)°1/2 106299.401
1800.815 Hg II 70 - 5d9.6s2 2D3/2 50555.567 5d9.6s.6p (2D<5/2>,1P<1>)°3/2 106086.013
1825.121 Hg II - - 5d9.6s.6p (2D<5/2>,3P<1>)°5/2 84836.143 5d10.9d 2D3/2 139627.043
1832.556 Hg II - -
1832.57 Hg I - - 5d10.6s.6p 31 39412.237 5d10.6p2 3P1 93980
1849.4994 Hg I 5000 - 5d10.6s2 1S0 0 5d10.6s.6p 11 54068.6829
1862.233 Hg II - -
1868.064 Hg II - -
1869.228 Hg II 405 - 5d10.6p 21/2 51486.07 5d10.6d 2D3/2 104984.138
1870.781 Hg II - -
1870.957 Hg II - - 5d9.6s.6p (2D<5/2>,3P<1>)°3/2 86178.478 5d10.9d 2D3/2 139627.043
1875.55 Hg II 15 - 5d9.6s2 2D3/2 50555.567 5d9.6s.6p (2D<3/2>,3P<1>)°1/2 103873.302
1877. Hg I 30 - 5d10.6s.6p 32 44042.909 5d9.6s2.(2D5/2).7s 2[5/2]2 97309.84
1885. Hg I 35 - 5d10.6s.6p 32 44042.909 5d9.6s2.(2D5/2).7s 2[5/2]3 97100.23
1894.77 Hg III - -
1900.121 Hg II 4 - 5d9.6s2 2D3/2 50555.567 5d9.6s.6p (2D<3/2>,3P<1>)°3/2 103183.874
1902.609 Hg II - - 5d9.6s.6p (2D<5/2>,3P<2>)°3/2 94092.834 5d9.6p2 (2D<5/2>,3P<0>)5/2 146652.263
1915.943 Hg II - - 5d9.6s.6p (2D<5/2>,1P<1>)°7/2 106215.059 5d9.6p2 (2D<5/2>,3P<2>)7/2 158408.647
1917. Hg I 8 - 5d10.6s.6p 32 44042.909 5d10.6p2 3P2 96190
1929.04 Hg II - - 5d9.6s.6p (2D<5/2>,1P<1>)°3/2 106086.013 5d9.6p2 (2D<5/2>,3P<2>)5/2 157925.207
1934.591 Hg II - - 5d9.6s.6p (2D<5/2>,1P<1>)°7/2 106215.059 5d9.6p2 (2D<5/2>,3P<2>)9/2 157905.52
1942.2729 Hg II 420 - 5d10.6s 2S1/2 0 5d10.6p 21/2 51486.07
1947.491 Hg II - - 5d9.6s.6p (2D<5/2>,3P<2>)°5/2 95304.138 5d9.6p2 (2D<5/2>,3P<0>)5/2 146652.263
1972.87 Hg I 4 - 5d10.6s.6p 31 39412.237 5d10.6p2 3P0 90099.6
1973.794 Hg II 55 - 5d9.6s2 2D5/2 35514.624 5d9.6s.6p (2D<5/2>,3P<1>)°3/2 86178.478
1980.702 Hg II - - 5d9.6s.6p (2D<5/2>,3P<1>)°7/2 84212.404 5d10.8d 2D5/2 134699.466
1987.841 Hg II 35 - 5d9.6s2 2D3/2 50555.567 5d9.6s.6p (2D<3/2>,3P<1>)°5/2 100861.369
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