TITANIUM (22)

The spectrum of titanium is so rich in lines, and is so largely represented in stellar spectra, that a tabulation would occupy an undue amount of space.

[TABLE XI]

SeriesWave-Lenght Int. Cl. Attribution Int. Wave-Lenght
3613.8460II-, Sc43613.947
3645.3130IIISc?, -33645.475
3630.7650II 43630.876
3666.543III13666.676
3651.8125III-, Sc43651.940
3642.7940IISc23642.912
3572.5350II-, Sc63572.71
3558.5520II(Fe83558.672)
3590.4820II23590.609
3576.3535II-, Sc?33576.527
3567.7020II43567.835
3589.6420II53589.773
3580.9430II53581.067
5657.8925V EY, -25658.09
5684.2112V E15684.415
5640.9915V E25641.206
5667.169V E05667.368
5658.358V E05658.561
5669.0510V E15669.258
4374.4640III ESc, Fe?33374.628
4420.662004420.832
4354.605V E14354.776
4400.3830III ESc34400.555
4431.353V E04431.525
4384.806IV E04384.986
4415.5520III E24415.722
4314.0960III ESc34314.248
4294.778IV EZr24294.932
4320.7350III ESc34320.90
4279.951------
4305.7010IV E24305.871
4325.0040III ESc44325.152

From an examination of Rowland’s tables of the solar spectrum, it appears that the fainter components of the multiplets invariably accompany the stronger ones, thus making the identifications certain. Only the stronger components are, however, powerful enough to appear in stellar spectra, with the dispersions ordinarily used.

The following multiplets, as analyzed by Russell[290] and Kiess,[291] are definitely present:

,

,