2014
DOI: 10.1063/1.4863559
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Omni-conducting and omni-insulating molecules

Abstract: The source and sink potential model is used to predict the existence of omni-conductors (and omniinsulators): molecular conjugated π systems that respectively support ballistic conduction or show insulation at the Fermi level, irrespective of the centres chosen as connections. Distinct, ipso, and strong omni-conductors/omni-insulators show Fermi-level conduction/insulation for all distinct pairs of connections, for all connections via a single centre, and for both, respectively. The class of conduction behavio… Show more

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Cited by 23 publications
(87 citation statements)
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“…A molecular graph with nullity ≤ 1 may be a distinct omni-conductor; if it has nullity ≥ 2, it may be a distinct omni-insulator. 45 This dichotomy ultimately derives from the mathematics of the interlacing theorem, 48 as deletion of two vertices of a graph can change its nullity by at most two.…”
Section: Introductionmentioning
confidence: 99%
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“…A molecular graph with nullity ≤ 1 may be a distinct omni-conductor; if it has nullity ≥ 2, it may be a distinct omni-insulator. 45 This dichotomy ultimately derives from the mathematics of the interlacing theorem, 48 as deletion of two vertices of a graph can change its nullity by at most two.…”
Section: Introductionmentioning
confidence: 99%
“…It follows, for example, that significant classes of conjugated hydrocarbons, such as the Kekulean benzenoids, cannot be distinct omni-conductors. 45 Hence, it is natural to ask how closely an alternant hydrocarbon can approach omni-conductor or omni-insulator status. The present paper gives a systematic answer to this question by defining near omniconduction and insulation and showing that there are only a very few possible cases needed to describe real π systems.…”
Section: Introductionmentioning
confidence: 99%
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