Premium
A symmetry adapted approach to the dynamic Jahn‐Teller problem: Application to mixed‐valence polyoxometalate clusters with keggin structure
Author(s) -
Tsukerblat Boris,
Palii Andrew,
ClementeJuan Juan M.,
GaitaAriño Alejandro,
Coronado Eugenio
Publication year - 2012
Publication title -
international journal of quantum chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.484
H-Index - 105
eISSN - 1097-461X
pISSN - 0020-7608
DOI - 10.1002/qua.24152
Subject(s) - delocalized electron , irreducible representation , hamiltonian (control theory) , jahn–teller effect , basis set , valence (chemistry) , vibronic coupling , singlet state , electronic structure , quantum mechanics , physics , chemistry , ion , mathematics , excited state , density functional theory , mathematical optimization
In this article, we present a symmetry‐adapted approach aimed to the accurate solution of the dynamic vibronic problem in large scale Jahn‐Teller (JT) systems. The algorithm for the solution of the eigen‐problem takes full advantage of the point symmetry arguments. The system under consideration is supposed to consist of a set of electronic levels mixed by the active JT and pseudo JT vibrational modes. Applying the successive coupling of the bosonic creation operators, we introduce the irreducible tensors that are called multivibronic operators. Action of the irreducible multivibronic operators on the vacuum state creates the vibrational symmetry adapted basis that is subjected to the Gram‐Schmidt orthogonalization at each step of evaluation. Finally, the generated vibrational basis is coupled to the electronic one to get the symmetry adapted electron‐vibrational (vibronic) basis within which the full matrix of the JT Hamiltonian is blocked according to the irreducible representations (irreps) of the point group. The proposed approach is a part of our study of the nanosized mixed valence (MV) clusters with large number of delocalized electrons that are at the border line between quantum and classical objects. Here, we illustrate in detail the developed technique by the application to the 2e‐reduced MV dodecanuclear Keggin anion in which the electronic pair is delocalized over 12 sites (overall symmetry T d ) giving rise to the ( 1 T 2 + 1 E + 1 A 1 )⊗( e + t 2 ) ( 3 T 1 + 3 T 2 )⊗( e + t 2 ) combined JT/pseudo JT problems for the spin‐singlet and spin‐triplet states. © 2012 Wiley Periodicals, Inc.