General treatment of the multimode Jahn-Teller effect: study of fullerene cations
A general model for the analysis of the Adiabatic Potential Energy Surfaces (APES) of the molecules that are subject to the multimode Jahn-Teller effect is presented. The method utilizes the information obtained by DFT calculations on a distorted stationary point on the APES. The essence of the mode...
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Published in | Physical chemistry chemical physics : PCCP Vol. 15; no. 4; pp. 1252 - 1259 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
Cambridge
Royal Society of Chemistry
28.01.2013
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Subjects | |
Online Access | Get full text |
ISSN | 1463-9076 1463-9084 1463-9084 |
DOI | 10.1039/c2cp43591h |
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Summary: | A general model for the analysis of the Adiabatic Potential Energy Surfaces (APES) of the molecules that are subject to the multimode Jahn-Teller effect is presented. The method utilizes the information obtained by DFT calculations on a distorted stationary point on the APES. The essence of the model is to express the distortion along a model minimal energy path called Intrinsic Distortion Path (IDP), projecting the geometry of the system on the normal modes of the either high-symmetry (HS) or low symmetry (LS) nuclear configuration. This allows us to determine the significance of all of the involved normal modes along a relevant particular path of distortion, and the direct calculation of the vibronic coupling constants. The IDP analysis is illustrated by the discussion of the multimode H ⊗ (g + 2h) JT effect in fullerene cations (C
60
+
) giving a deep insight into the origin and the mechanism of vibronic coupling in fullerene based molecules.
A general approach, fully non-empirical, to analyse the multimode distortion using multideterminantal-DFT and Intrinsic Distortion Path methods has been presented and illustrated on C
60
+
. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 ObjectType-Article-2 ObjectType-Feature-1 |
ISSN: | 1463-9076 1463-9084 1463-9084 |
DOI: | 10.1039/c2cp43591h |