{ "id": "1001.1834", "version": "v1", "published": "2010-01-12T09:54:38.000Z", "updated": "2010-01-12T09:54:38.000Z", "title": "Beryllium abundances and the formation of the halo and the thick disk", "authors": [ "R. Smiljanic", "L. Pasquini", "P. Bonifacio", "D. Galli", "B. Barbuy", "R. Gratton", "S. Randich" ], "comment": "6 pages, 5 figures, To appear in the Proceedings of IAU Symp. 268 - Light Elements in the Universe (C. Charbonnel, M. Tosi, F. Primas, C. Chiappini, eds)", "categories": [ "astro-ph.SR", "astro-ph.GA" ], "abstract": "The single stable isotope of beryllium is a pure product of cosmic-ray spallation in the ISM. Assuming that the cosmic-rays are globally transported across the Galaxy, the beryllium production should be a widespread process and its abundance should be roughly homogeneous in the early-Galaxy at a given time. Thus, it could be useful as a tracer of time. In an investigation of the use of Be as a cosmochronometer and of its evolution in the Galaxy, we found evidence that in a log(Be/H) vs. [alpha/Fe] diagram the halo stars separate into two components. One is consistent with predictions of evolutionary models while the other is chemically indistinguishable from the thick-disk stars. This is interpreted as a difference in the star formation history of the two components and suggests that the local halo is not a single uniform population where a clear age-metallicity relation can be defined. We also found evidence that the star formation rate was lower in the outer regions of the thick disk, pointing towards an inside-out formation.", "revisions": [ { "version": "v1", "updated": "2010-01-12T09:54:38.000Z" } ], "analyses": { "keywords": [ "thick disk", "beryllium abundances", "star formation history", "halo stars separate", "single uniform population" ], "tags": [ "journal article" ], "publication": { "doi": "10.1017/S1743921310004667" }, "note": { "typesetting": "TeX", "pages": 6, "language": "en", "license": "arXiv", "status": "editable", "inspire": 842616, "adsabs": "2010IAUS..268..483S" } } }