Dielectric anisotropy in the GW space-time method

TY - JOUR

T1 - Dielectric anisotropy in the GW space-time method

AU - Freysoldt, C.

AU - Eggert, P.

AU - Schindlmayr, A.

AU - Godby, R.W.

AU - Scheffler, M.

AU - Rinke, P.

N1 - © 2006 Elsevier B.V. This is an author produced version of a paper published in Computer Physics Communications and uploaded in accordance with the publisher's self archiving policy.

PY - 2007/1/1

Y1 - 2007/1/1

N2 - Excited-state calculations, notably for quasiparticle band structures, are nowadays routinely performed within the GW approximation for the electronic self-energy. Nevertheless, certain numerical approximations and simplifications are still employed in practice to make the computations feasible. An important aspect for periodic systems is the proper treatment of the singularity of the screened Coulomb interaction in reciprocal space, which results from the slow 1/r decay in real space. This must be done without introducing artificial interactions between the quasiparticles and their periodic images in repeated cells, which occur when integrals of the screened Coulomb interaction are discretised in reciprocal space. An adequate treatment of both aspects is crucial for a numerically stable computation of the self-energy. In this article we build on existing schemes for isotropic screening and present an extension for anisotropic systems. We also show how the contributions to the dielectric function arising from the non-local part of the pseudopotentials can be computed efficiently. These improvements are crucial for obtaining a fast convergence with respect to the number of points used for the Brillouin zone integration and prove to be essential to make GW calculations for strongly anisotropic systems, such as slabs or multilayers, efficient. (C) 2006 Elsevier B.V. All rights reserved.

AB - Excited-state calculations, notably for quasiparticle band structures, are nowadays routinely performed within the GW approximation for the electronic self-energy. Nevertheless, certain numerical approximations and simplifications are still employed in practice to make the computations feasible. An important aspect for periodic systems is the proper treatment of the singularity of the screened Coulomb interaction in reciprocal space, which results from the slow 1/r decay in real space. This must be done without introducing artificial interactions between the quasiparticles and their periodic images in repeated cells, which occur when integrals of the screened Coulomb interaction are discretised in reciprocal space. An adequate treatment of both aspects is crucial for a numerically stable computation of the self-energy. In this article we build on existing schemes for isotropic screening and present an extension for anisotropic systems. We also show how the contributions to the dielectric function arising from the non-local part of the pseudopotentials can be computed efficiently. These improvements are crucial for obtaining a fast convergence with respect to the number of points used for the Brillouin zone integration and prove to be essential to make GW calculations for strongly anisotropic systems, such as slabs or multilayers, efficient. (C) 2006 Elsevier B.V. All rights reserved.

KW - GW approximation

KW - anisotropic screening

KW - Coulomb singularity

KW - dielectric function

KW - ELECTRONIC-STRUCTURE CALCULATIONS

KW - BAND-STRUCTURE CALCULATIONS

KW - DENSITY-FUNCTIONAL THEORY

KW - AB-INITIO CALCULATION

KW - SELF-ENERGY

KW - SEMICONDUCTORS

KW - EXCHANGE

KW - APPROXIMATION

KW - CONSTANT

KW - SOLIDS

U2 - 10.1016/j.cpc.2006.07.018

DO - 10.1016/j.cpc.2006.07.018

M3 - Article

VL - 176

SP - 1

EP - 13

JO - Computer Physics Communications

JF - Computer Physics Communications

SN - 0010-4655

IS - 1

ER -