Far-Infrared Observations of the Galactic Center

1970 ◽  
Vol 159 ◽  
pp. L159 ◽  
Author(s):  
H. H. Aumann ◽  
F. J. Low
1977 ◽  
Vol 216 ◽  
pp. 277 ◽  
Author(s):  
I. Gatley ◽  
E. E. Becklin ◽  
C. G. Wynn-Williams ◽  
M. W. Werner

1978 ◽  
Vol 220 ◽  
pp. 822 ◽  
Author(s):  
I. Gatley ◽  
E. E. Becklin ◽  
M. W. Werner ◽  
D. A. Harper

1980 ◽  
Vol 241 ◽  
pp. L183 ◽  
Author(s):  
P. M. Harvey ◽  
M. F. Campbell ◽  
W. F. Hoffmann

1976 ◽  
Vol 205 ◽  
pp. L69 ◽  
Author(s):  
P. M. Harvey ◽  
M. F. Campbell ◽  
W. F. Hoffmann

1996 ◽  
Vol 466 ◽  
pp. 242 ◽  
Author(s):  
Ralf Timmermann ◽  
Reinhard Genzel ◽  
Albrecht Poglitsch ◽  
Dieter Lutz ◽  
Suzanne C. Madden ◽  
...  

1979 ◽  
Vol 84 ◽  
pp. 367-375 ◽  
Author(s):  
E. R. Wollman

Infrared observations have provided considerable information about the structure and energetics of the galactic center. The stellar bulge dominates the mass and luminosity of the nuclear region. The luminosity of the bulge is strongly peaked toward the center, even within the central parsec. Dust in the nuclear disk absorbs the power output of the central portion of the bulge and reemits it in the far infrared. Near the center, molecular clouds move in a plane apparently tilted toward the Sun. Within the central few parsecs, or core, the inclination may be as large as 45°. The total power output of the core is about twice that of the bulge population alone. The source of excess luminosity is uncertain, but evidence points to ongoing star formation associated with the Sgr A molecular complex.


1997 ◽  
Vol 163 ◽  
pp. 725-726
Author(s):  
K.-W. Hodapp ◽  
E. F. Ladd

Stars in the earliest phases of their formation, i.e., those accreting the main component of their final mass, are deeply embedded within dense cores of dust and molecular material. Because of the high line-of-sight extinction and the large amount of circumstellar material, stellar emission is reprocessed by dust into long wavelength radiation, typically in the far-infrared and sub-millimeter bands. Consequently, the youngest sources are strong submillimeter continuum sources, and often undetectable as point sources in the near-infrared and optical. The most deeply embedded of these sources have been labelled “Class 0” sources by André, Ward-Thompson, & Barsony (1994), in an extension of the spectral energy distribution classification scheme first proposed by Adams, Lada, & Shu (1987).


1982 ◽  
Author(s):  
W. A. Dent ◽  
M. W. Werner ◽  
I. Gatley ◽  
E. E. Becklin ◽  
R. H. Hildebrand ◽  
...  

2020 ◽  
Author(s):  
Richard J. Bantges ◽  
Helen E. Brindley ◽  
Jonathan E. Murray ◽  
Alan E. Last ◽  
Cathryn Fox ◽  
...  

Abstract. Measurements of mid- to far-infrared nadir radiances obtained from the UK Facility for Airborne Atmospheric Measurements (FAAM) BAe-146 aircraft during the Cirrus Coupled Cloud-Radiation Experiment (CIRCCREX) are used to assess the performance of various ice cloud bulk optical (single-scattering) property models. Through use of a minimisation approach, we find that the simulations can reproduce the observed spectra in the mid-infrared to within measurement uncertainty but are unable to simultaneously match the observations over the far-infrared frequency range. When both mid and far-infrared observations are used to minimise residuals, first order estimates of the flux differences between the best performing simulations and observations indicate a strong compensation effect between the mid and far infrared such that the absolute broadband difference is


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