{ "id": "0809.0542", "version": "v1", "published": "2008-09-03T04:05:57.000Z", "updated": "2008-09-03T04:05:57.000Z", "title": "Alpha-Particle Condensation in Nuclear Systems", "authors": [ "Y. Funaki", "T. Yamada", "H. Horiuchi", "G. Röpke", "P. Schuck", "A. Tohsaki" ], "comment": "29 pages, 21 figures", "categories": [ "nucl-th" ], "abstract": "The onset of quartetting, i.e. alpha-particle condensation, in symmetric nuclear matter is studied with the help of an in-medium modified four nucleon equation. It is found that at very low density quartetting wins over pairing, because of the strong binding of the alpha-particles. The critical temperature can reach values up to around 6 MeV. Also the disappearance of alpha-particles with increasing density, i.e. the Mott transition, is investigated. In finite nuclei the Hoyle state, that is the 0_2^+ of 12C, is identified as an \"alpha-particle condensate\" state. It is conjectured that such states also exist in heavier n alpha-nuclei, like 16O, 20Ne, etc. For instance the 6-th 0^+ state of 16O at 15.1 MeV is identified from a theoretical analysis as being a strong candidate for an alpha condensate state. Exploratory calculations are performed for the density dependence of the alpha condensate fraction at zero temperature to address the suppression of the four-particle condensate below nuclear-matter density. Possible quartet condensation in other systems is discussed briefly", "revisions": [ { "version": "v1", "updated": "2008-09-03T04:05:57.000Z" } ], "analyses": { "keywords": [ "alpha-particle condensation", "nuclear systems", "alpha condensate state", "low density quartetting wins", "symmetric nuclear matter" ], "tags": [ "journal article" ], "publication": { "doi": "10.1088/1742-6596/413/1/012009" }, "note": { "typesetting": "TeX", "pages": 29, "language": "en", "license": "arXiv", "status": "editable", "inspire": 795521, "adsabs": "2008arXiv0809.0542F" } } }