Please use this identifier to cite or link to this item: http://nopr.niscpr.res.in/handle/123456789/29239
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dc.contributor.authorDelarue, Patrice-
dc.contributor.authorSenet, Patrick-
dc.date.accessioned2014-08-08T10:51:18Z-
dc.date.available2014-08-08T10:51:18Z-
dc.date.issued2014-08-
dc.identifier.issn0975-0975(Online); 0376-4710(Print)-
dc.identifier.urihttp://hdl.handle.net/123456789/29239-
dc.description1052-1057en_US
dc.description.abstractThe charge distribution induced by an inhomogeneous electric potential applied to a molecule is in fact the sum of two terms: polarization (localized) and chemical (delocalized) charge distributions. The chemical induced charge distribution is proportional to the inhomogeneous response of the molecule to an electron transfer (Fukui function). Analogy with the electrostatic Thomson theorem for the perfect conductors permits to define the quantum molecular capacitance. en_US
dc.language.isoen_USen_US
dc.publisherNISCAIR-CSIR, Indiaen_US
dc.rights CC Attribution-Noncommercial-No Derivative Works 2.5 Indiaen_US
dc.sourceIJC-A Vol.53A(08-09) [August-September 2014]en_US
dc.subjectTheoretical chemistryen_US
dc.subjectDensity functional calculationsen_US
dc.subjectPolarizationen_US
dc.subjectChemical reactivityen_US
dc.subjectElectrostaticsen_US
dc.subjectQuantum molecular capacitanceen_US
dc.subjectFukui functionen_US
dc.titlePolarization, reactivity and quantum molecular capacitance: From electrostatics to density functional theoryen_US
dc.typeArticleen_US
Appears in Collections:IJC-A Vol.53A(08-09) [August-September 2014]

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