Abstract:We devise a mixing algorithm for full-potential (FP) all-electron calculations in the linearized augmented planewave (LAPW) method. Pulay’s direct inversion in the iterative subspace is complemented with the Kerker preconditioner and further improvements to achieve smooth convergence, avoiding charge sloshing and noise in the exchange–correlation potential. As the Kerker preconditioner was originally designed for the planewave basis, we have adapted it to the FP-LAPW method and implemented in the exciting code… Show more
“…In the previous Section 2.2 the interstitial Yukawa potential is used as boundary values for the Yukawa potential in the atomic spheres. This subsection is concerned with the construction of the Fourier transformable pseudo-charge density ρ α that replaces the true local charge density ρ α [see (11)] inside the muffin-tin sphere such that the Yukawa potential in the interstitial region,…”
Section: Interstitial Yukawa Potentialmentioning
confidence: 99%
“…By solving Eq. 1 for general periodic densities, the Kerker preconditioner [9] can be extended to density functional methods of general densities [10,11].…”
We present a general method for solving the modified Helmholtz equation without shape approximation for an arbitrary periodic charge distribution, whose solution is known as the Yukawa potential or the screened Coulomb potential. The method is an extension of Weinert’s pseudo-charge method [Weinert M, J Math Phys, 1981, 22:2433–2439] for solving the Poisson equation for the same class of charge density distributions. The inherent differences between the Poisson and the modified Helmholtz equation are in their respective radial solutions. These are polynomial functions, for the Poisson equation, and modified spherical Bessel functions, for the modified Helmholtz equation. This leads to a definition of a modified pseudo-charge density and modified multipole moments. We have shown that Weinert’s convergence analysis of an absolutely and uniformly convergent Fourier series of the pseudo-charge density is transferred to the modified pseudo-charge density. We conclude by illustrating the algorithmic changes necessary to turn an available implementation of the Poisson solver into a solver for the modified Helmholtz equation.
“…In the previous Section 2.2 the interstitial Yukawa potential is used as boundary values for the Yukawa potential in the atomic spheres. This subsection is concerned with the construction of the Fourier transformable pseudo-charge density ρ α that replaces the true local charge density ρ α [see (11)] inside the muffin-tin sphere such that the Yukawa potential in the interstitial region,…”
Section: Interstitial Yukawa Potentialmentioning
confidence: 99%
“…By solving Eq. 1 for general periodic densities, the Kerker preconditioner [9] can be extended to density functional methods of general densities [10,11].…”
We present a general method for solving the modified Helmholtz equation without shape approximation for an arbitrary periodic charge distribution, whose solution is known as the Yukawa potential or the screened Coulomb potential. The method is an extension of Weinert’s pseudo-charge method [Weinert M, J Math Phys, 1981, 22:2433–2439] for solving the Poisson equation for the same class of charge density distributions. The inherent differences between the Poisson and the modified Helmholtz equation are in their respective radial solutions. These are polynomial functions, for the Poisson equation, and modified spherical Bessel functions, for the modified Helmholtz equation. This leads to a definition of a modified pseudo-charge density and modified multipole moments. We have shown that Weinert’s convergence analysis of an absolutely and uniformly convergent Fourier series of the pseudo-charge density is transferred to the modified pseudo-charge density. We conclude by illustrating the algorithmic changes necessary to turn an available implementation of the Poisson solver into a solver for the modified Helmholtz equation.
“…They were originally devised for planewave based methods. Recent theoretical studies have shown a formulation of the Kerker preconditioner as well as its implementation in full-potential (FP) calculations with the linearized augmented planewave (LAPW) basis set [26,27]. The Resta preconditioner, however, is not yet reformulated to implement in the FP-LAPW method.…”
Section: Introductionmentioning
confidence: 99%
“…In practice, strong fluctuations in ρ out i caused by a small change of ρ in i prevent the convergence during the self-consistency iteration. This phenomenon is well-known as charge sloshing [17][18][19][20][21][22][23][24][25][26][27], which is more severe in metals with large supercells. To avoid this problem, one can add an effective preconditioner in Eq.…”
Section: Introductionmentioning
confidence: 99%
“…Based on this method, thus, the Hartree potential can be evaluated. Several studies have shown that it is still available for solving the screened Poisson equation [26,27,41]. Tran et al used this method for the implementation of screened hybrid functionals [41].…”
Convergence in self-consistent-field cycles can be a major computational bottleneck of densityfunctional theory calculations. We propose a Resta-like preconditioning method for full-potential all-electron calculations in the linearized augmented planewave (LAPW) method to smoothly converge to self-consistency. We implemented this preconditioner in the exciting code and apply it to the two semiconducting systems of MoS2 slabs and P-rich GaP(100) surfaces as well as the metallic system Au(111), containing a sufficiently large amount of vacuum. Our calculations demonstrate that the implemented scheme performs reliably as well as more efficiently regardless of system size, suppressing long-range charge sloshing. While the suitability of this preconditioning higher for semiconducting systems, the convergence for metals is only slightly decreased and thus still trustworthy to apply. Furthermore, a mixing algorithm with the preconditioner shows an improvement over that with the Kerker preconditioner for the investigated semiconducting systems.
PRECONDITIONERS: KERKER AND RESTAThe simplest mixing approach is to linearly mix the previous input and output charge density. In this case, a
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