1984Monthly Notices of the Royal Astronomical SocietyOpen access

Shocked molecular hydrogen emission from the centre of the Galaxy

I. Gatley, T. J. Jones, A. R. Hyland, D. H. Beattie, T. J. Lee

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Abstract

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.

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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.

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Available abstract

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

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