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Accretion of low-metallicity gas by the Milky Way

B. P. Wakker (), J. C. Howk, B. D. Savage, H. van Woerden, S. L. Tufte, U. J. Schwarz, R. Benjamin, R. J. Reynolds, R. F. Peletier and P. M. W. Kalberla
Additional contact information
B. P. Wakker: Department of Astronomy
J. C. Howk: The Johns Hopkins University
B. D. Savage: Department of Astronomy
H. van Woerden: Kapteyn Institute
S. L. Tufte: Lewis & Clark College
U. J. Schwarz: Kapteyn Institute
R. Benjamin: University of Wisconsin
R. J. Reynolds: Department of Astronomy
R. F. Peletier: University of Durham
P. M. W. Kalberla: Radio-astronomisches Institüt Universität Bonn

Nature, 1999, vol. 402, issue 6760, 388-390

Abstract: Abstract Models of the chemical evolution of the Milky Way suggest that the observed abundances of elements heavier than helium (‘metals’) require a continuous infall of gas with metallicity (metal abundance) about 0.1 times the solar value. An infall rate integrated over the entire disk of the Milky Way of ∼1 solar mass per year can solve the ‘G-dwarf problem’—the observational fact that the metallicities of most long-lived stars near the Sun lie in a relatively narrow range1,2,3. This infall dilutes the enrichment arising from the production of heavy elements in stars, and thereby prevents the metallicity of the interstellar medium from increasing steadily with time. However, in other spiral galaxies, the low-metallicity gas needed to provide this infall has been observed only in associated dwarf galaxies4 and in the extreme outer disk of the Milky Way5,6. In the distant Universe, low-metallicity hydrogen clouds (known as ‘damped Lyα absorbers’) are sometimes seen near galaxies7,8. Here we report a metallicity of 0.09 times solar for a massive cloud that is falling into the disk of the Milky Way. The mass flow associated with this cloud represents an infall per unit area of about the theoretically expected rate, and ∼0.1–0.2 times the amount required for the whole Galaxy.

Date: 1999
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DOI: 10.1038/46498

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