The the common element in methods known as multi-level computer simulations is the use of different basic physical descriptors of a complex investigated systems for different length- and/or time-scales. Our interest lies in methods, which use orbital-type of descriptors for a selected part of a larger system and simpler descriptors elswhere. The highest level is indispensabe to describe phenomena of essentialy quantum mechanical nature (chemical bonds, electronic spectroscopy).
We are especially interested in first-principles based description of the frontier between the subsystem described at the orbital level and its environment. A non-empirical formalism based on a mixed description of the whole system by means of embedded orbitals and electron density introduced in [T.A. Wesolowski and A. Warshel J. Phys. Chem. 97 (1993) 8050], which we refer to as: orbital-free embedding formalism
, makes it possible to link the orbital-level description with any other type of theory provided it yields the electron density of the environment. In multi-level simulations based on this formalism, the embedded orbitals are obtained from Kohn-Sham-like equations (i.e. one-electron equations with a multiplicative effective potential). This effective embeding potential is expressed by means of the electron density in the environment. Any method, which yields the electron density as a function of position in space, can be used to generate the effective embedding potential.Opposite to commonly used methods in quantum chemistry labeled as QM/MM or QM/MD, orbital-free embedding simulations do not involve any system-specific parameters because the effective embedding potential is expressed by means of universal density functionals. In the exact-functional limit, the orbital-free embedding formalism leads to the exact ground-state electron density. The results of practical orbital-free embedding calculations are not exact due to the use of approximate density functionals of the non-additive kinetic energy and exchange-correlation energy instead of the exact ones. Approximations to the bi-functional of the non-additive kinetic energy are also needed in subsystem formulation of density functional theory , whereas approximating the exchange-correlation energy is indispensable methods based on Kohn-Sham formulation. Our work on density functional theory focuses on studies of approximations to these functionals in order to improve the currently used ones and/or to determine their range of applicability. Currently, the approximate functionals allow us to study reliebly such embedded systems, which interact with their environment without forming covalent bonds.
Xiuwen Zhou, Jakub W. Kaminski, Tomasz A. Wesolowski Phys. Chem. Chem. Phys. , 13 (2011) 10565-10576 (special issue on Multilevel Modelling).
Jakub W. Kaminski, Sergey Gusarov, Andriy Kovalenko, Tomasz A. Wesolowski Journal of Physical Chemistry A , 114 (2010) 6082.
T.A. Wesolowski, Computational Chemistry: Reviews of Current Trends - Vol. 10 World Scientific, 2006, pp. 1-82.
J. Neugebauer, M.J. Louwerse, P. Belanzoni, T.A. Wesolowski, E. J. Baerends, J. Chem. Phys. 123 (2005) 114101.
J. Neugebauer, C.R. Jacob, T.A. Wesolowski, E.J. Baerends, J. Phys. Chem. A. 109 (2005) 7805.
J. Neugebauer, M.J. Louwerse, E.J. Baerends, T.A. Wesolowski, J. Chem. Phys. 122 (2005) 094115
G. Hong, M. Strajbl, T.A. Wesolowski, and A. Warshel, J. Comput. Chem., 21 (2000) 1554.
R.P. Muller, T. Wesolowski, and A. Warshel, In: Density functional methods: Applications in chemistry and materials science., M. Springborg, ed. John Wiley and Sons, Ltd. (1997) pp.189-206
T.A. Wesolowski, R. Muller, and A. Warshel, J. Phys. Chem. 100 (1996) 15444.
T.A. Wesolowski and A. Warshel, J. Phys. Chem. 98 (1994) 5183.
T.A. Wesolowski and A. Warshel J. Phys. Chem. 97 (1993) 8050.