Shocked molecular hydrogen emission from the centre of the Galaxy
I. Gatley, T. J. Jones, A. R. Hyland, D. H. Beattie, T. J. Lee
Abstract
Open-access reader
I. Gatley, T. J. Jones, A. R. Hyland, D. H. Beattie, T. J. Lee
Abstract
Open-access reader
Observations of molecular hydrogen emission lines near 2 µm show that the nucleus of the Galaxy is encircled by a ring of shocked gas; this ring has a radius of 2 parsecs, lies in the plane of the Galaxy, is symmetric about the centre of mass, and rotates in the sense of Galactic rotation. Gas is being shocked at a rate of |$\gt 10^{-2} M_\odot \enspace \text {yr}^{-1}$| to a temperature about 2000 K, in a region of mean molecular density |$5 \times 10^3 \text {cm}^{-3}$|. The momentum needed to shock the gas cannot be provided radiatively. Mass loss from the nucleus can account naturally for the central density minimum and for the shocked gas; a mass loss rate of |$3 \times 10^{-3} M_\odot \enspace \text {yr}^{-1}$| is required. Simple time-scale arguments suggest that observable molecular hydrogen emission from the Galactic centre may be a long-lived phenomenon. A model involving a single central engine is suggested.
OpenAlex reports 45 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
Observations of molecular hydrogen emission lines near 2 µm show that the nucleus of the Galaxy is encircled by a ring of shocked gas; this ring has a radius of 2 parsecs, lies in the plane of the Galaxy, is symmetric about the centre of mass, and rotates in the sense of Galactic rotation. Gas is being shocked at a rate of |$\gt 10^{-2} M_\odot \enspace \text {yr}^{-1}$| to a temperature about 2000 K, in a region of mean molecular density |$5 \times 10^3 \text {cm}^{-3}$|. The momentum needed to shock the gas cannot be provided radiatively. Mass loss from the nucleus can account naturally for the central density minimum and for the shocked gas; a mass loss rate of |$3 \times 10^{-3} M_\odot \enspace \text {yr}^{-1}$| is required. Simple time-scale arguments suggest that observable molecular hydrogen emission from the Galactic centre may be a long-lived phenomenon. A model involving a single central engine is suggested.
Key concepts: Physics, Astrophysics, Galaxy, RADIUS, Molecular cloud, Galaxy rotation curve, Hydrogen molecule, Hydrogen