scholarly journals Mid-Infrared Hydrogen Recombination Line Emission From the Maser Star MWC 349A

1997 ◽  
Vol 114 ◽  
pp. 2658 ◽  
Author(s):  
Howard A. Smith ◽  
V. Strelnitski ◽  
J. W. Miles ◽  
D. M. Kelly ◽  
J. H. Lacy
1974 ◽  
Vol 60 ◽  
pp. 81-85
Author(s):  
F. J. Kerr ◽  
P. D. Jackson ◽  
G. R. Knapp ◽  
R. L. Brown

This paper reports two new recombination-line results. The first is the detection of carbon line emission from the dark cloud near ϱ Ophiuchi, and the second discusses the origin of hydrogen recombination line emission associated with ionized gas outside known discrete continuum sources.


1998 ◽  
Vol 184 ◽  
pp. 91-92 ◽  
Author(s):  
D. Lutz

Since its launch in November 1995, the Infrared Space Observatory ISO has converted mid-infrared spectroscopy into a mature tool. Due to its proximity, brightness, and the wealth of complementary information, the center of our Galaxy remains a unique testbed for studies of galactic nuclei. A first analysis of the 2.4-45μm spectrum obtained with ISO-SWS (Fig. 1) has been presented by Lutz et al. (1996a). One of the surprises is a determination of the mid-infrared extinction law from comparison of the Galactic center hydrogen recombination line fluxes and case B expectations: The extinction law clearly lacks the deep minimum near 7μm expected for standard graphite/silicate mixes. External galaxies are less close to the ideal ‘screen’ case and cannot provide the detail of the GC recombination line spectrum needed to derive an extinction law. However, simple ratios of the strongest recombination lines are inconsistent with a classical extinction law and any dust configuration.


2016 ◽  
Vol 11 (S322) ◽  
pp. 21-24
Author(s):  
Elena Murchikova

AbstractThe submm Hydrogen recombination line technique can be used as a probe of the Galactic Center. We present the results of our H30α observations of ionized gas from within 0.015 pc around SgrA*. The observations were obtained on ALMA in cycle 3. The line was not detected, but we were able to set a limit on the mass of the cool gas (T~ 104 K) at 2 × 10−3M⊙. This is the unique probe of gas cooler than T ~106 K traced by X-ray emission. The total amount of gas near SgrA* gives us clues to understanding the accretion rate of SgrA*.


1973 ◽  
Vol 183 ◽  
pp. L143 ◽  
Author(s):  
Diego A. Cesarsky ◽  
Catherine J. Cesarskly

1972 ◽  
Vol 239 (95) ◽  
pp. 126-126 ◽  
Author(s):  
B. G. LESLIE ◽  
W. A. DENT

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