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141.
L. M. Hobbs 《Monthly notices of the Royal Astronomical Society》2005,359(4):1356-1362
The effects of the hyperfine structure (HFS) that is present in some interstellar absorption lines are investigated in the case of a single absorbing cloud. If the respective total equivalent widths of two or more unresolved HFS multiplets measured in relatively low-resolution spectra are analysed specifically by means of a curve of growth, the column density N (X) and the linewidth parameter b (X) inferred for absorbing species X in the cloud will generally be in error if the HFS is ignored. The fundamental physical effect is the reduced line saturation that arises because the total column density is divided among the HFS levels of the ground atomic level, each of which generally gives rise to an HFS line at a different wavelength. For nuclear spins I = 3/2 and I = 5/2 , theoretical curves of growth are calculated for some of the resonance lines of some alkali atoms, for each of four illustrative choices of the parameter α=Δ/ b , the ratio of the HFS splitting in the ground atomic level to the linewidth. Applications of the results to interstellar absorption by Na i , K i and Al iii are emphasized. HFS is, fortunately, unimportant for most interstellar lines, however. Among the 35 elements that have been detected in diffuse clouds via interstellar absorption in the ultraviolet/optical spectral region, the most abundant isotope of each of 25 of these shows no HFS, because I = 0 or, in the relevant ground atomic level, J = 0 . 相似文献
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This review describes advances in radiative transfer theory since about 1985. We stress fundamental aspects and emphasize
modern methods for the numerical solution of the transfer equation for spatially multidimensional problems, for both unpolarized
and polarized radiation. We restrict the discussion to two-level atoms with noninverted populations for given temperature,
density and velocity fields.
Unfortunately this article was originally published with typesetter's errors: The correct publication date was 25 February
2006, not 3 January 2006. The content was not in the final form. The publishers wish to apologize for this mistake. The online
version of the original version can be found at /10.1007/s00159-005-0025-8. 相似文献
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148.
Rekhesh Mohan K. S. Dwarakanath G. Srinivasan Jayaram N. Chengalur 《Journal of Astrophysics and Astronomy》2001,22(1):35-50
Nearby interstellar clouds with high (|ν|≥10km s−1) random velocities although easily detected in NaI and CaII lines have hitherto not been detected (in emission or absorption)
in the HI 21cm line. We describe here deep Giant Metrewave Radio Telescope (GMRT) HI absorption observations toward radio
sources with small angular separation from bright O and B stars whose spectra reveal the presence of intervening high random
velocity CaII absorbing clouds. In 5 out of the 14 directions searched we detect HI 21cm absorption features from these clouds.
The mean optical depth of these detections is ∼0.09 and FWHM is ∼10km s−1, consistent with absorption arising from CNM clouds. 相似文献
149.
A. Niezurawska M. Szymczak A. M. S. Richards R. J. Cohen 《Astrophysics and Space Science》2005,295(1-2):37-42
Two star-forming regions Cepheus A and W75N, were searched for the 4765-MHz OH maser emission using the multi-element radio linked interferometer network (MERLIN). The excited OH emission has an arc-like structure of 40 mas in Cep A and a linear structure of size 45 mas in W75N. We also found the 1720-MHz line in Cep A and Hutawarakorn [MNRAS 330 (2002) 349] reported the 1720-MHz emission in W75N. The 1720- and 4765-MHz OH spots coincided in space within 60 mas and in velocity within 0.3 km s–1 in both targets implying that both maser transitions arise from the same region. According to the modelling by Gray [MNRAS 252 (1991) 30] the 1720/4765-MHz co-propagation requires a low density, warm environment. The masers lie at the edges of H II regions where such conditions are expected. 相似文献
150.
A. Peraiah 《Journal of Astrophysics and Astronomy》1980,1(1):3-16
Comoving frame calculations have been used to compute the spectral lines formed in rapidly expanding spherical media. We have
employed the angle-averaged partial frequency redistribution functionR
I with a two-level atom model in non-LTE atom approximation. A linear velocity law increasing with radius has been employed
with maximum velocity at Τ=0 being set equal to 30 mean thermal units. It is found that one obtains almost symmetric emission
line profiles at large velocities similar to those found in quasars. 相似文献