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arXiv:cond-mat/9805246 · Computer Physics Communications

The GW space-time method for the self-energy of large systems

Martin M. Rieger, Lutz Steinbeck, I.D. White, H. Rojas, Rex W. Godby

Published Mar 1, 1999• 177 citations
arXivHTMLPDF
DOI
10.1016/s0010-4655(98)00174-x

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Within the framework of many-body perturbation theory based on Green's functions, the GW approximation has emerged as a pivotal method for computing quasiparticle energies and excitation spectra. However, its high computational cost and steep scaling present significant challenges for applications to large molecular systems. In this work, we extend the block tensor decomposition (BTD) algorithm, recently developed in our previous work [Zhang et al., J. Chem. Phys. 163, 174109 (2025)] for low-rank tensor compression, to enable a formally O(N3)-scaling GW algorithm. By integrating BTD with an imaginary-time GW formalism and introducing a real space screening strategy for the polarizability, we achieve an observed scaling of approximately O(N2) in test systems. Key parameters of the algorithm are optimized on the S66 dataset using the JADE algorithm, ensuring a balanced compromise between accuracy and efficiency. Our BTD-based random phase approximation also exhibits O(N2) scaling, and eigenvalue-self-consistent GW calculations become feasible for systems with over 3000 basis functions. This work establishes BTD as an efficient and scalable approach for large-scale GW calculations in molecular systems.
We present a method to calculate the GW self-energy in which no summation over the empty states appears. We obtain an explicit expression for the matrix elements of the self-energy in frequency space that does not contain any reference to the empty states. Our method yields a hierarchy of equations for the self-energy. The expressions for the self-energy thus obtained are very simple and can be readily implemented leading to an immediate speedup of GW calculations. Truncation of this hierarchy at low order already leads to excellent results for the quasiparticle energies.