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The SIESTA method for ab initio order-N materials simulation

The SIESTA method for ab initio order-N materials simulation We have developed and implemented a selfconsistent densityfunctional method using standard norm-conservingpseudopotentials and a flexible, numericallinear combination of atomic orbitals basis set,which includes multiple-zeta and polarization orbitals.Exchange and correlation are treated with the local spin densityor generalized gradient approximations. The basis functions andthe electron density are projected on a real-space grid, inorder to calculate the Hartree and exchange-correlation potentials and matrix elements, with a number of operations thatscales linearly with the size of the system. We use a modifiedenergy functional, whose minimization produces orthogonalwavefunctions and the same energy and density as the Kohn-Shamenergy functional, without the need for an explicitorthogonalization. Additionally, using localized Wannier-likeelectron wavefunctions allows the computation time and memoryrequired to minimize the energy to also scale linearly withthe size of the system. Forces and stresses are also calculatedefficiently and accurately, thus allowing structural relaxationand molecular dynamics simulations. http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Journal of Physics: Condensed Matter IOP Publishing

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Copyright
Copyright © IOP Publishing Ltd
ISSN
0953-8984
eISSN
1361-648X
DOI
10.1088/0953-8984/14/11/302
Publisher site
See Article on Publisher Site

Abstract

We have developed and implemented a selfconsistent densityfunctional method using standard norm-conservingpseudopotentials and a flexible, numericallinear combination of atomic orbitals basis set,which includes multiple-zeta and polarization orbitals.Exchange and correlation are treated with the local spin densityor generalized gradient approximations. The basis functions andthe electron density are projected on a real-space grid, inorder to calculate the Hartree and exchange-correlation potentials and matrix elements, with a number of operations thatscales linearly with the size of the system. We use a modifiedenergy functional, whose minimization produces orthogonalwavefunctions and the same energy and density as the Kohn-Shamenergy functional, without the need for an explicitorthogonalization. Additionally, using localized Wannier-likeelectron wavefunctions allows the computation time and memoryrequired to minimize the energy to also scale linearly withthe size of the system. Forces and stresses are also calculatedefficiently and accurately, thus allowing structural relaxationand molecular dynamics simulations.

Journal

Journal of Physics: Condensed MatterIOP Publishing

Published: Mar 8, 2002

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