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
4019.6321	Pb	I	4	-	6s2.6p2	(3/2,3/2)2	21457.7982	6s2.6p.(2P°1/2).6d	2[5/2]°3	46328.6668
4031.16	Pb	III	7	-
4049.8	Pb	IV	2	-
4057.8067	Pb	I	4000	108	6s2.6p2	(3/2,1/2)2	10650.3271	6s2.6p.7s	(1/2,1/2)°1	35287.2244
4062.136	Pb	I	35	1	6s2.6p2	(3/2,3/2)2	21457.7982	6s2.6p.(2P°1/2).6d	2[3/2]°1	46068.4385
4094.54	Pb	III	7	-
4110.76	Pb	II	15	1
4113.35	Pb	II	15	1
4128.11	Pb	III	70	7
4152.82	Pb	II	345	47
4157.8144	Pb	I	80	13	6s2.6p2	(3/2,3/2)0	29466.8303	6s2.6p.9s	(1/2,1/2)°1	53511.1485
4168.0328	Pb	I	1500	248	6s2.6p2	(3/2,3/2)2	21457.7982	6s2.6p.(2P°1/2).6d	2[5/2]°2	45443.171
4242.14	Pb	II	105	38
4244.92	Pb	II	1000	409	6s2.6d	2D5/2	68964.31	6s2.5f	2F°7/2	92515.24
4272.66	Pb	III	240	104
4293.82	Pb	II	20	9
4296.65	Pb	II	15	8
4340.41258	Pb	I	285	136	6s2.6p2	(3/2,3/2)0	29466.8303	6s2.6p.(2P°1/2).7d	2[3/2]°1	52499.6391
4352.74	Pb	II	225	103
4386.46	Pb	II	1500	732	6s2.6d	2D3/2	69739.603	6s2.5f	2F°5/2	92530.66
4496.15	Pb	IV	120	57
4499.34	Pb	III	120	60
4534.6	Pb	IV	465	234
4571.21	Pb	III	255	129
4579.051	Pb	II	75	38
4582.27	Pb	II	75	38
4596.45	Pb	III	8	4
4605.4	Pb	IV	20	9
4761.12	Pb	III	135	84
4798.59	Pb	III	135	88
4809.36	Pb	V	7	4
4826.86	Pb	III	6	4
4855.06	Pb	III	6	4
5005.41642	Pb	I	1000	822	6s2.6p2	(3/2,3/2)0	29466.8303	6s2.6p.7s	(3/2,1/2)°1	49439.6165
5006.5724	Pb	I	-	-	6s2.6p.7s	(1/2,1/2)°0	34959.9084	6s2.6p.9p	(1/2,3/2)1	54928.0835
5042.58	Pb	II	285	233	6s2.7p	2P°1/2	74458.99	6s2.7d	2D3/2	94284.58
5065.12	Pb	III	5	4
5070.58	Pb	II	180	150
5074.53	Pb	II	180	147
5076.352	Pb	I	4	4	6s2.6p.7s	(1/2,1/2)°0	34959.9084	6s2.6p.9p	(1/2,1/2)1	54653.72
5089.48355	Pb	I	-	-	6s2.6p.7s	(1/2,1/2)°1	35287.2244	6s2.6p.9p	(1/2,3/2)2	54930.1086
5090.008	Pb	I	-	-	6s2.6p.7s	(1/2,1/2)°1	35287.2244	6s2.6p.9p	(1/2,3/2)1	54928.0835
5107.2423	Pb	I	5	4	6s2.6p.7s	(1/2,1/2)°1	35287.2244	6s2.6p.9p	(1/2,1/2)0	54861.806
5111.64	Pb	II	6	5
5191.56	Pb	III	65	59
5201.43711	Pb	I	360	320	6s2.6p2	(3/2,3/2)0	29466.8303	6s2.6p.8s	(1/2,1/2)°1	48686.934
5367.64	Pb	II	9	9
5372.099	Pb	II	420	403
5523.97	Pb	III	3	3
5544.25	Pb	II	3	3

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