Stellar atmospheres : $b A contribution to the observational study of high temperature in the reversing layers of starsPayne-Gaposchkin, Cecilia
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Stellar atmospheres : $b A contribution to the observational study of high temperature in the reversing layers of stars
Payne-Gaposchkin, Cecilia
Astrophysics; Stars -- Spectra; Stars -- Temperature; Thesis (Ph. D.)
The series relations for the arc spectrum of cobalt[324] have been
published by Walters. Cobalt lines are frequent in the solar spectrum,
but as the strongest of them lie near 3500, they cannot be traced in
the spectra of stars. The following multiplets are certainly identified
in the spectrum of the sun: , , ,
, , , , ,
, , and . The incompletely observed
multiplet is apparently absent from the solar spectrum.
NICKEL (28)
The series relations for nickel are as yet unpublished. The lines
appear in great numbers in the solar spectrum, but they are not strong
enough to be conspicuous in the spectra of the stars. The line 5476
appears to have a maximum at , indicating either that it is
an enhanced line of nickel, or that it is blended with the enhanced
line of some other element. The lines 5081, 4714 are strengthened in
low temperature stars, and are probably due to neutral nickel. From
the solar behavior of the lines of this element,[325] the ionization
potential seems to be of the same order as that for cobalt, probably
about 8 volts.
COPPER (29)
Copper is represented in the solar spectrum by the ultimate doublet
3273, 3247 (), which is strong. The pair 5700, 5782
() is probably also present. The former lines are too far
in the ultra-violet to have been studied in the stars, and the latter
are too faint.
ZINC (30)
The principal singlet is at 2138, and has therefore not
been observed in stellar spectra. The lines at 4722,
4810, are seen in the stellar sequence, where they appear at ,
and have a maximum[326] at .
[Pg 81]
Two unclassified lines of ionized zinc are mentioned in Fowler’s Report
as lying at 5894, 6214. Neither of these lines can be traced in solar
or stellar spectra.
GALLIUM (31)
The occurrence of gallium in stellar spectra is confined to the
identification of two solar lines by Hartley and Ramage.[327] The
lines in question are at 4033, 4172, and are the ultimate lines of the
element (). They are too faint to be studied in the
stars.
RUBIDIUM (37)
The ultimate lines of rubidium have been detected in the sunspot
spectrum,[328] but they are not found in the spectra of the sun or
stars.
STRONTIUM (38)
The element strontium is of great astrophysical importance, owing to
the use of its enhanced lines in the estimation of absolute magnitudes.
The neutral atom is represented in the sun and stars by the ultimate
line () 4607, which is first clearly seen[329] at ,
and increases progressively in strength with advancing type. It varies
with absolute magnitude, being weakened in stars of high luminosity
later than . Estimates for the intensity of this line are
difficult with small dispersions, as it is blended in cool stars.
IONIZED STRONTIUM
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