Universal tight binding model for chemical reactions in solution and at surfaces. I. Organic molecules

被引:8
作者
Sheppard, T. J. [1 ]
Lozovoi, A. Y. [1 ]
Pashov, D. L. [2 ]
Kohanoff, J. J. [1 ]
Paxton, A. T. [2 ]
机构
[1] Queens Univ Belfast, Sch Math & Phys, Atomist Simulat Ctr, Belfast BT7 1NN, Antrim, North Ireland
[2] Kings Coll London, Dept Phys, London WC2R 2LS, England
基金
英国工程与自然科学研究理事会;
关键词
DENSITY-FUNCTIONAL THEORY; ORBITAL THEORY; SEMIEMPIRICAL METHODS; DIFFERENTIAL-OVERLAP; GROUND-STATES; DIPOLE-MOMENT; BOND; PARAMETERS; APPROXIMATIONS; OPTIMIZATION;
D O I
10.1063/1.4887095
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
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. (C) 2014 AIP Publishing LLC.
引用
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页数:16
相关论文
共 52 条
[1]  
Andersen O. K., 1984, Electronic Structure of Complex Systems. Proceedings of a NATO Advanced Study Institute, P11
[2]  
[Anonymous], COULSONS VALENCE
[3]   GROUND-STATES OF MOLECULES .26. MINDO-3 CALCULATIONS FOR HYDROCARBONS [J].
BINGHAM, RC ;
DEWAR, MJS ;
LO, DH .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 1975, 97 (06) :1294-1301
[4]   Nonsingular Hankel functions as a new basis for electronic structure calculations [J].
Bott, E ;
Methfessel, M ;
Krabs, W ;
Schmidt, PC .
JOURNAL OF MATHEMATICAL PHYSICS, 1998, 39 (06) :3393-3425
[5]   Ab initio molecular dynamics study of the keto-enol tautomerism of acetone in solution [J].
Cucinotta, Clotilde S. ;
Ruini, Alice ;
Catellani, Alessandra ;
Stirling, Andras .
CHEMPHYSCHEM, 2006, 7 (06) :1229-1234
[6]   GROUND-STATES OF MOLECULES .38. MNDO METHOD - APPROXIMATIONS AND PARAMETERS [J].
DEWAR, MJS ;
THIEL, W .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 1977, 99 (15) :4899-4907
[7]   THE DEVELOPMENT AND USE OF QUANTUM-MECHANICAL MOLECULAR-MODELS .76. AM1 - A NEW GENERAL-PURPOSE QUANTUM-MECHANICAL MOLECULAR-MODEL [J].
DEWAR, MJS ;
ZOEBISCH, EG ;
HEALY, EF ;
STEWART, JJP .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 1985, 107 (13) :3902-3909
[8]   Self-consistent-charge density-functional tight-binding method for simulations of complex materials properties [J].
Elstner, M ;
Porezag, D ;
Jungnickel, G ;
Elsner, J ;
Haugk, M ;
Frauenheim, T ;
Suhai, S ;
Seifert, G .
PHYSICAL REVIEW B, 1998, 58 (11) :7260-7268
[9]   Relative energetics and structural properties of zirconia using a self-consistent tight-binding model [J].
Fabris, S ;
Paxton, AT ;
Finnis, MW .
PHYSICAL REVIEW B, 2000, 61 (10) :6617-6630
[10]  
Finnis M., 2003, INTERATOMIC FORCES C