7.1.5 Interstellar absorption lines and bands in stellar spectra

Author(s):  
H. Scheffler
1999 ◽  
Vol 193 ◽  
pp. 80-81
Author(s):  
Joy S. Nichols ◽  
Jeffrey L. Linsky

The NEWSIPS-reprocessing of IUE data permits the extraction of spectra to wavelengths as short as 1150 Å. We present representative well-exposed IUE spectra of Wolf-Rayet stars covering the 1150–1220 Å region with a resolution of 0.1 Å. The C III 1175 Å line in WC and some WN stars typically shows a P-Cygni profile, with dacs apparent in time series spectra. Superimposed on the stellar spectra are many strong interstellar absorption lines of N I, Si II and other species. These spectra are a guide to a portion of the wavelength region to be covered by FUSE, and an indication of the new information that will be available in the far-UV range with FUSE.


1957 ◽  
Vol 4 ◽  
pp. 66-66
Author(s):  
R. S. Lawrence

The detailed relationship between optical interstellar absorption lines and 21-cm. observations is investigated in this paper.Dr Guido Münch, of the Mount Wilson and Palomar Observatories, provided the list of six intermediate-latitude stars shown in Table 1. The spectra of these stars all show complex absorption lines due to interstellar Ca 11. The 21-cm. line is measurable in four of the six regions, although the peak intensity is low in each case. It is noteworthy that for the first two stars on the list the radio velocity agrees closely with the velocity of an intense optical component. In view of the great difference in angular resolution, the failure to find correspondence in every case is not surprising.


1933 ◽  
Vol 4 ◽  
pp. 175-177
Author(s):  
M. H. N. Russell ◽  
MM. Abetti ◽  
Adams ◽  
J. Baillaud ◽  
Bosler ◽  
...  

Investigation of stellar spectra has been active during the last four years. Without attempting to make a complete survey, some important researches may be mentioned.The theory of the intensities and contours of absorption lines has been discussed by Eddington, Milne, Pannekoek, Woolley, H. H. Plaskett, and others, and has proved to be difficult. For example, no quantitative theory has yet been developed for the residuai intensity which remains in even the strongest lines, although the physical causes underlying the formation of residual intensities are rather obvious. Study of solar lines with light which has left the surface at different angles shows that the processes which produce the wings and the centre are probably different. The most promising line of attack on this intricate problem appears to be in studies of the solar spectrum, where different regions of the disc may be separately investigated, rather than of integrated starlight. The highest dispersion available, even in solar work, will be none too great.


1994 ◽  
Vol 214 (1-2) ◽  
pp. 93-102
Author(s):  
L. Semionova ◽  
Jorge P�ez ◽  
J. Bonatti

1983 ◽  
Vol 274 ◽  
pp. 136 ◽  
Author(s):  
D. G. York ◽  
C. C. Wu ◽  
J. C. Blades ◽  
S. Ratcliff ◽  
L. L. Cowie ◽  
...  

1990 ◽  
Vol 351 ◽  
pp. 412 ◽  
Author(s):  
D. G. York ◽  
A. Caulet ◽  
P. Rybski ◽  
J. Gallagher ◽  
J. C. Blades ◽  
...  

1977 ◽  
Vol 4 (2) ◽  
pp. 363-364
Author(s):  
Yoji Kondo

The Mg II resonance lines at 2795.523 and 2802.698Å and their respective subordinate lines at 2797.989 and 2790.768Å are probably among the most prominent and interesting spectral features in the ultraviolet; they are perhaps the most significant in the mid-ultraviolet. They are also observable in one form or the other in stars of practically all spectral types. We shall discuss relatively high (about 0.4Å) resolution observations of these features.In the early spectral types both the resonance and subordinate lines are seen primarily as absorption lines. An interstellar absorption of varying strengths is superimposed on the photospheric absorption of the resonance lines. The strengths of the photospheric resonance and subordinate lines increase from 0 to B, e.g., Lamers et al. (1973) and Kondo et al. (1975). The subordinate lines begin to merge with the resonance lines in late-B stars. In mid-A type stars, the resonance and subordinate absorption strengths become maximum. In F-type stars, the photospheric absorption strenghts continue to decrease. Chromospheric emissions become definitely detectable in F-type stars (Kondo et al. 1972). In a G2 V star, the sun, the chromospheric emission is fairly prominent at the core of relatively weak photospheric absorption. In K and M-type stars, this region is presumably dominated by the chromospheric emissions of Mg II resonance lines with the photospheric absorption becoming negligible in late-K stars; the only extant observation in this region is that of e Eri (K2 V) (McClintock et al. 1975).


Sign in / Sign up

Export Citation Format

Share Document