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Stochastic Density Functional Theory Through the Lens of Multilevel Monte Carlo Method

Xue Quan, Huajie Chen

TL;DR

The paper addresses the high cost of traditional Kohn–Sham DFT by employing stochastic density functional theory (sDFT) with random orbitals and Chebyshev expansions. It introduces a multilevel Monte Carlo (MLMC) framework to reduce variance and decouple cost from discretization size and temperature, via two hierarchical decompositions: energy cutoffs and polynomial orders. The authors provide rigorous variance bounds and show, through numerical experiments on graphene-like systems, that MLMC can achieve significant cost reductions while preserving accuracy, with the total work scaling as $O(n^{(0)} N M)$ or $O(n^{(0)} N M^{(0)})$, independent of the finest discretization or smearing parameter. This work therefore offers a theoretically grounded, scalable route for large-scale electronic structure calculations using sDFT.

Abstract

The stochastic density functional theory (sDFT) has exhibited advantages over the standard Kohn-Sham DFT method and has become an attractive approach for large-scale electronic structure calculations. The sDFT method avoids the expensive matrix diagonalization by introducing a set of random orbitals and approximating the density matrix via Chebyshev expansion of a matrix-valued function. In this work, we study the sDFT with a plane-wave discretization, and discuss variance reduction algorithms in the framework of multilevel Monte Carlo (MLMC) methods. In particular, we show that the density matrix evaluation in sDFT can be decomposed into many levels by increasing the plane-wave cutoffs or the Chebyshev polynomial orders. This decomposition renders the computational cost independent of the discretization size or temperature. To demonstrate the efficiency of the algorithm, we provide rigorous analysis of the statistical errors and present numerical experiments on some material systems.

Stochastic Density Functional Theory Through the Lens of Multilevel Monte Carlo Method

TL;DR

The paper addresses the high cost of traditional Kohn–Sham DFT by employing stochastic density functional theory (sDFT) with random orbitals and Chebyshev expansions. It introduces a multilevel Monte Carlo (MLMC) framework to reduce variance and decouple cost from discretization size and temperature, via two hierarchical decompositions: energy cutoffs and polynomial orders. The authors provide rigorous variance bounds and show, through numerical experiments on graphene-like systems, that MLMC can achieve significant cost reductions while preserving accuracy, with the total work scaling as or , independent of the finest discretization or smearing parameter. This work therefore offers a theoretically grounded, scalable route for large-scale electronic structure calculations using sDFT.

Abstract

The stochastic density functional theory (sDFT) has exhibited advantages over the standard Kohn-Sham DFT method and has become an attractive approach for large-scale electronic structure calculations. The sDFT method avoids the expensive matrix diagonalization by introducing a set of random orbitals and approximating the density matrix via Chebyshev expansion of a matrix-valued function. In this work, we study the sDFT with a plane-wave discretization, and discuss variance reduction algorithms in the framework of multilevel Monte Carlo (MLMC) methods. In particular, we show that the density matrix evaluation in sDFT can be decomposed into many levels by increasing the plane-wave cutoffs or the Chebyshev polynomial orders. This decomposition renders the computational cost independent of the discretization size or temperature. To demonstrate the efficiency of the algorithm, we provide rigorous analysis of the statistical errors and present numerical experiments on some material systems.

Paper Structure

This paper contains 19 sections, 6 theorems, 91 equations, 2 figures.

Key Result

Lemma 3.1

Let $\chi\in\mathbb{C}^n$ be the random orbital satisfying ass:randorb. Then Moreover, if $\chi$ additionally satisfiesAmong the three random orbital examples provided below equation ass:randorb, both (a) and (b) satisfy this additional condition, while (c) does not -- $\chi_i$ follows a normal distribution with the fourth moment $\mathbb{E}[|\chi_i|^4]=3$. then

Figures (2)

  • Figure 1: Atomic configurations of the grahene-type systems. (a) Perfect lattice. (b) Stone-Wales defect. (c) Boron (blue) / nitrogen (red) doped graphene.
  • Figure 4: Variance across levels for multilevel energy cutoffs.

Theorems & Definitions (14)

  • Lemma 3.1
  • Remark 3.2: $L^2$-error of the electron density
  • Remark 3.3: Cost scaling
  • Lemma 4.1
  • Remark 4.2: Cost reduction by MLMC
  • Theorem 4.3
  • Remark 4.4: Cost scaling for multilevel on energy cutoffs
  • Theorem 4.5
  • Remark 4.6: Cost scaling for multilevel on polynomial orders
  • Lemma A.1
  • ...and 4 more