As is now well established, a first order expansion of the Hohenberg–Kohn total energy density functional about a trial input density, namely, the Harris–Foulkes functional, can be used to rationalize a non self consistent tight binding model. If the expansion is taken to second order then the energy and electron density matrix need to be calculated self consistently and from this functional one can derive a charge self consistent tight binding theory. In this paper we have used this to describe a polarizable ion tight binding model which has the benefit of treating charge transfer in point multipoles. This admits a ready description of ionic polarizability and crystal field splitting. It is necessary in constructing such a model to find a number of parameters that mimic their more exact counterparts in the density functional theory. We describe in detail how this is done using a combination of intuition, exact analytical fitting, and a genetic optimization algorithm. Having obtained model parameters we show that this constitutes a transferable scheme that can be applied rather universally to small and medium sized organic molecules. We have shown that the model gives a good account of static structural and dynamic vibrational properties of a library of molecules, and finally we demonstrate the model's capability by showing a real time simulation of an enolization reaction in aqueous solution. In two subsequent papers, we show that the model is a great deal more general in that it will describe solvents and solid substrates and that therefore we have created a self consistent quantum mechanical scheme that may be applied to simulations in heterogeneous catalysis.
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28 July 2014
Research Article|
July 28 2014
Universal tight binding model for chemical reactions in solution and at surfaces. I. Organic molecules Available to Purchase
T. J. Sheppard;
T. J. Sheppard
1Atomistic Simulation Centre, School of Mathematics and Physics,
Queen's University Belfast
, Belfast BT7 1NN, Northern Ireland, United Kingdom
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A. Y. Lozovoi;
A. Y. Lozovoi
1Atomistic Simulation Centre, School of Mathematics and Physics,
Queen's University Belfast
, Belfast BT7 1NN, Northern Ireland, United Kingdom
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D. L. Pashov;
D. L. Pashov
2Department of Physics,
King's College London
, Strand, London WC2R 2LS, United Kingdom
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J. J. Kohanoff;
J. J. Kohanoff
1Atomistic Simulation Centre, School of Mathematics and Physics,
Queen's University Belfast
, Belfast BT7 1NN, Northern Ireland, United Kingdom
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A. T. Paxton
A. T. Paxton
a)
2Department of Physics,
King's College London
, Strand, London WC2R 2LS, United Kingdom
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T. J. Sheppard
1
A. Y. Lozovoi
1
D. L. Pashov
2
J. J. Kohanoff
1
A. T. Paxton
2,a)
1Atomistic Simulation Centre, School of Mathematics and Physics,
Queen's University Belfast
, Belfast BT7 1NN, Northern Ireland, United Kingdom
2Department of Physics,
King's College London
, Strand, London WC2R 2LS, United Kingdom
a)
Author to whom correspondence should be addressed. Electronic mail: [email protected].
J. Chem. Phys. 141, 044503 (2014)
Article history
Received:
April 17 2014
Accepted:
June 25 2014
Connected Content
A companion article has been published:
Universal tight binding model for chemical reactions in solution and at surfaces. II. Water
Citation
T. J. Sheppard, A. Y. Lozovoi, D. L. Pashov, J. J. Kohanoff, A. T. Paxton; Universal tight binding model for chemical reactions in solution and at surfaces. I. Organic molecules. J. Chem. Phys. 28 July 2014; 141 (4): 044503. https://doi.org/10.1063/1.4887095
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