{ "id": "cond-mat/0206328", "version": "v3", "published": "2002-06-18T19:31:39.000Z", "updated": "2002-10-30T21:23:34.000Z", "title": "Current-voltage Characteristics of Molecular Conductors: Two versus Three Terminal", "authors": [ "Prashant Damle", "Titash Rakshit", "Magnus Paulsson", "Supriyo Datta" ], "comment": "9 pages, 9 figures. Major changes in text. One new result added (Fig 8). Accepted for publication in IEEE Trans. on Nanotechnology", "doi": "10.1109/TNANO.2002.806825", "categories": [ "cond-mat.mes-hall" ], "abstract": "This paper addresses the question of whether a ``rigid molecule'' (one which does not deform in an external field) used as the conducting channel in a standard three-terminal MOSFET configuration can offer any performance advantage relative to a standard silicon MOSFET. A self-consistent solution of coupled quantum transport and Poisson's equations shows that even for extremely small channel lengths (about 1 nm), a ``well-tempered'' molecular FET demands much the same electrostatic considerations as a ``well-tempered'' conventional MOSFET. In other words, we show that just as in a conventional MOSFET, the gate oxide thickness needs to be much smaller than the channel length (length of the molecule) for the gate control to be effective. Furthermore, we show that a rigid molecule with metallic source and drain contacts has a temperature independent subthreshold slope much larger than 60 mV/decade, because the metal-induced gap states in the channel prevent it from turning off abruptly. However, this disadvantage can be overcome by using semiconductor contacts because of their band-limited nature.", "revisions": [ { "version": "v3", "updated": "2002-10-30T21:23:34.000Z" } ], "analyses": { "keywords": [ "current-voltage characteristics", "molecular conductors", "rigid molecule", "temperature independent subthreshold slope", "gate oxide thickness needs" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable" } } }