dc.contributor.author | Moulopoulos, Konstantinos | en |
dc.creator | Moulopoulos, Konstantinos | en |
dc.date.accessioned | 2019-12-02T15:32:00Z | |
dc.date.available | 2019-12-02T15:32:00Z | |
dc.date.issued | 2000 | |
dc.identifier.uri | http://gnosis.library.ucy.ac.cy/handle/7/58891 | |
dc.description.abstract | By using an accurate dielectric function for a homogeneous paramagnetic electron liquid we attempt a simple analytical treatment of the bound-state (metal-insulator) transition in a system consisting of a single proton immersed in the electron liquid, as a function of global density. The inability of the resulting effective Thomas-Fermi picture to account for the transition is remedied by the inclusion of the appropriate cusp condition that is also introduced in a simple analytical manner. The expected transition from a delocalized state (at high density) to a localized state (at low density) is shown to be the result of the combined action of a minimal number of very general principles such as overall charge neutrality, the compressibility sum rule and the so-called q4 sum rule, at the simplest analytical level. © 2000 IOP Publishing Ltd. | en |
dc.source | Journal of Physics Condensed Matter | en |
dc.source.uri | https://www.scopus.com/inward/record.uri?eid=2-s2.0-24044546843&doi=10.1088%2f0953-8984%2f12%2f7%2f312&partnerID=40&md5=b7d0d5f8de32d0906efe9d5a87663c27 | |
dc.title | Bound-state transition: An analytical model | en |
dc.type | info:eu-repo/semantics/article | |
dc.identifier.doi | 10.1088/0953-8984/12/7/312 | |
dc.description.volume | 12 | |
dc.description.issue | 7 | |
dc.description.startingpage | 1285 | |
dc.description.endingpage | 1296 | |
dc.author.faculty | Σχολή Θετικών και Εφαρμοσμένων Επιστημών / Faculty of Pure and Applied Sciences | |
dc.author.department | Τμήμα Φυσικής / Department of Physics | |
dc.type.uhtype | Article | en |
dc.source.abbreviation | J Phys Condens Matter | en |
dc.contributor.orcid | Moulopoulos, Konstantinos [0000-0001-5139-436X] | |
dc.gnosis.orcid | 0000-0001-5139-436X | |