Projection based embedding theory for solving Kohn-Sham density functional theory
For computational chemists and materials scientists, PET offers a potentially exact embedding method with reduced cost, but the contribution is incremental as it builds on existing theory with a perturbation correction.
The paper reformulates projection based embedding theory (PET) for Kohn-Sham DFT from a linear algebra perspective, enabling reduced computational cost by confining calculations to a system part. A first-order perturbation correction improves accuracy, achieving sufficient precision even for strong perturbations, e.g., computing SiH3F ground state energy using SiH4 as reference.
Quantum embedding theories are playing an increasingly important role in bridging different levels of approximation to the many body Schrödinger equation in physics, chemistry and materials science. In this paper, we present a linear algebra perspective of the recently developed projection based embedding theory (PET) [Manby et al, J. Chem. Theory Comput. 8, 2564, 2012], restricted to the context of Kohn-Sham density functional theory. By partitioning the global degrees of freedom into a `system' part and a `bath' part, and by choosing a proper projector from the bath, PET is an in principle exact formulation to confine the calculation to the system part only, and hence can be carried out with reduced computational cost. Viewed from the perspective of the domain decomposition method, one particularly interesting feature of PET is that it does not enforce a boundary condition explicitly, and remains applicable even when the discretized Hamiltonian matrix is dense, such as in the context of the planewave discretization. In practice, the accuracy of PET depends on the accuracy of the projector for the bath. Based on the linear algebra reformulation, we develop a first order perturbation correction to the projector from the bath to improve its accuracy. Numerical results for real chemical systems indicate that with a proper choice of reference system, the perturbatively corrected PET can be sufficiently accurate even when strong perturbation is applied to very small systems, such as the computation of the ground state energy of a SiH$_3$F molecule, using a SiH$_4$ molecule as the reference system.