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
8563.59	Kr	II	-	-	4s2.4p4.(1D).5p	2P°3/2	150201.68	4s2.4p4.(3P).6s	4P1/2	161875.62
8563.93	Sc	I	20	-	3d.4s.(1D).4p	2P°3/2	24656.866	3d3	2D25/2	36330.537
8564.57	Th	I	-	-	5f.6d2.7s	5H°5	18011.3803	5f.6d.7s.7p	5H5	26380.54194
8564.7	Xe	I	-	-	5p5.(2P°3/2).5d	2[3/2]°1	83889.971	5p5.(2P°3/2).7f	2[3/2]2	95562.546
8564.71	As	I	90	-	4s2.4p2.(3P).5s	4P3/2	51610.2	4s2.4p2.(3P).5p	4P°5/2	63282.8
8564.889	Ge	I	15	-	4s2.4p.4d	3D°1	48962.783	4s2.4p.(2P°1/2).6f	2[5/2]2	60635.152
8565.1	Xe	II	-	-	5p4.(3P1).4f	2[3]°7/2	149682.65	5p4.(3P1).5g	2[4]9/2	161354.8
8565.25	Ba	III	4	-	5p5.(2P°3/2).6d	2[7/2]°4	218225	5p5.(2P°3/2).5f	2[7/2]4	229896.89
8565.34	Ar	II	2	-	3s2.3p4.(3P).3d	4F3/2	143371.4364	3s2.3p4.(3P).4p	4P°5/2	155043.1619
8565.488	Ti	I	85	-	3d3.(4P).4s	a 5P2	14028.436	3d2.(3P).4s.4p.(3P°)	5D°2	25699.987
8565.817	Mn	II	270	-	3d5.(6S).5p	x 7P°4	86057.625	3d5.(6S).6s	7S3	97728.727
8565.96	Ti	II	3	-	3d3	b 4F7/2	1087.3561	3d3	b 2D25/2	12758.2597
8566.24	Ti	III	7	-	3p6.3d.5d	3F3	169769.13	3p6.3d.5f	3H°4	181439.64
8566.282	Br	I	-	-	4s2.4p4.(3P2).5p	2[3]°7/2	75521.5	4s2.4p4.(3P2).5d	2[4]9/2	87191.97
8566.7	Xe	II	1	-	5p4.(3P2).4f	2[5]°11/2	139782	5p4.(3P2).5g	2[5]11/2	151451.3
8567.435	Ba	I	25	-	5d.6p	3D°2	24531.513	5d.6d	3D2	36200.412
8567.63	Pr	III	20	-
8567.74	N	I	195	-	2s2.2p2.(3P).3s	2P1/2	86137.35	2s2.2p2.(3P).3p	2P°3/2	97805.84
8567.79	Fe	I	-	-	3d6.(5D).4s.4p.(1P°)	x 5D°4	39625.804	3d6.(5D).4s (4D).5s	e 3D3	51294.22
8568.2089	Th	II	1	-	5f.(2F°).6d2.(3F)	4I°13/2	18816.8664	5f2.(3H).7s	2H11/2	30484.71231
8568.41	Rb	II	2	-	4p5.(2P°3/2).6p	2[1/2]0	189365.923	4p5.(2P°3/2).6d	2[3/2]°1	201033.495
8568.419	Fe	III	-	-	3d5.(6S).6p	7P°4	198737.2	3d5.(6S).6d	7D4	210404.8
8568.483	V	I	6	-	3d4.(3D).4s	b 4D5/2	20789.112	3d3.(2P).4s.4p.(3P°)	x 4D°3/2	32456.581
8568.83	Cf	II	10000	-
8569.02	Kr	I	2	-	4s2.4p5.(2P°3/2).4d	2[1/2]°0	96771.494	4s2.4p5.(2P°1/2).6p	2[3/2]1	108438.2603
8569.738	Ti	I	165	-	3d3.(2P).4s	b 3P0	17995.487	3d2.(3F).4s.4p.(1P°)	w 3D°1	29661.25
8570.099	Fe	I	-	-	3d6.(5D).4s (6D).5s	e 5D1	45509.152	3d6.4s.(6D).6p	7F°1	57174.43
8570.52	U	I	270	-
8570.8332	Fe	II	-	-	3d6.(3H).5s	e 4H13/2	98130.136	3d5.(2G2).4s.4p.(3P°)	4H°11/2	109794.406
8571.3535	Ne	I	90	-	2s2.2p5.(2P°1/2).3p	2[3/2]1	150772.1118	2s2.2p5.(2P°1/2).3d	2[3/2]°1	162435.678
8571.8047	Fe	I	-	-	3d6.(5D).4s.4p.(1P°)	x 5D°1	40404.518	3d6.(5D).4s (6D).4d	e 5P2	52067.469
8572.25	In	II	-	-	5s.6p	1P°1	109780.221	5s.7s	3S1	121442.541
8572.3	S	IV	-	-	3s.3p.(1P°).3d	2D°5/2	281231.6	3s.3p.(3P°).4p	2P3/2	292893.9
8572.438	Fe	II	-	-	3d6.(5D3).4f	2[3]°7/2	103385.785	3d6.(5D).6d	6P5/2	115047.887
8572.542	Sb	I	2000	-	5p2.(3P).6s	2P1/2	46991.058	5p2.(3P2).6p	(2,3/2)°1/2	58653.011
8572.655	Ne	II	75	-	2s2.2p4.(3P).3d	4P3/2	280989.5229	2s2.2p4.(3P).4p	4S°3/2	292651.298
8572.96	Pa	I	10000	-
8573.12042	Th	I	40	-	6d3.(4F).7s	5F1	5563.141519	6d2.7s.7p	5F°2	17224.30234
8573.53	Ti	III	1	-	3p6.3d.4f	1F°3	159180.24	3p6.3d.5d	1D2	170840.8
8573.592	V	I	3	-	3d4.(1G2).4s	b 2G7/2	21646.42	3d3.(2G).4s.4p.(3P°)	y 2G°9/2	33306.943
8574.093	Cu	II	-	-	3d8.(3F).4s.4p.(1P°)	3F°4	134742.863	3d9.(2D5/2).6d	2[9/2]5	146402.715
8574.7	W	I	15	-
8575.24	Cl	I	2	-	3s2.3p4.(3P).4s	4P1/2	72827.038	3s2.3p4.(3P).4p	4D°3/2	84485.309
8575.32	Co	I	85	-
8575.6736	V	I	4	-	3d4.(5D).4s	a 6D3/2	2153.221	3d3.4s2	a 2P1/2	13810.91
8575.87	Nb	I	65	-
8575.92	Ta	I	50	-	5d4.(5D).6s	a 6D9/2	13351.45	5d3.6s.(5F).6p	z 6G°11/2	25008.83
8576.01	Xe	I	105	-	5p5.(2P°1/2).6s	2[1/2]°1	77185.041	5p5.(2P°3/2).7p	2[1/2]0	88842.256
8577.	C	I	-	-	2s.2p3	3P°0	75256.1696	2s2.2p.6p	1P1	86912.89
8577.124	Fe	II	-	-	3d5.4s2	b 4G5/2	54275.649	3d6.(3G).4p	x 4G°7/2	65931.358

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