pith. machine review for the scientific record. sign in

arxiv: 2605.11512 · v1 · submitted 2026-05-12 · ❄️ cond-mat.mtrl-sci

Recognition: 2 theorem links

· Lean Theorem

G⁰W⁰ implementation based on the pseudopotential and numerical-atomic-orbital basis-set framework: Algorithms and benchmarks

Bohan Jia, Huanjing Gong, Lixin He, Min-Ye Zhang, Peize Lin, Xinguo Ren, Ziqing Guan

Authors on Pith no claims yet

Pith reviewed 2026-05-13 01:53 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci
keywords G0W0 methodnumerical atomic orbitalspseudopotentialsband structuredielectric functionrandom phase approximationlocalized resolution of identityquasiparticle energies
0
0 comments X

The pith

A G0W0 implementation within the numerical atomic orbital and pseudopotential framework reaches benchmark agreement with established codes through a compressed resolution of identity and analytic small-q handling.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

This paper sets out to deliver a working periodic G0W0 method inside the numerical-atomic-orbital plus pseudopotential setting that is already common in density functional calculations. It introduces a localized resolution of identity approach equipped with a new compression scheme that lowers cost and improves numerical stability, together with an analytic treatment of the small-wavevector limit that cuts the need for dense sampling. A practical check based on the frequency-dependent macroscopic dielectric function is offered to pick suitable pseudopotentials ahead of the G0W0 run. Systematic tests on band structures and gaps show close matches to other implementations, indicating that the approach can support calculations on systems larger than those typically handled in this basis.

Core claim

The central claim is that an NAO-PP G0W0 framework can be realized efficiently by combining the localized resolution of identity with a novel compression scheme, an analytic small-q treatment of the microscopic dielectric function, and real-space tensor filtering. These ingredients, together with a dielectric-function test for pseudopotential selection, produce quasiparticle band structures and gaps in excellent agreement with established G0W0 codes while delivering substantial computational gains.

What carries the argument

The localized resolution of identity (LRI) technique with a novel compression scheme, which reduces the cost of building the screened Coulomb interaction in the random phase approximation while preserving stability and accuracy.

If this is right

  • G0W0 calculations become feasible for larger periodic systems within the NAO-PP basis than was previously practical.
  • The analytic small-q treatment lowers the density of q-points required for converged dielectric functions.
  • A dielectric-function inspection provides a concrete route to select appropriate pseudopotentials before performing G0W0.
  • Real-space tensor filtering yields additional efficiency gains without degrading benchmark agreement.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same compression and filtering steps could be reused in other many-body perturbation methods that rely on the random phase approximation.
  • The NAO flexibility may simplify GW studies of low-dimensional or defective structures where plane-wave convergence is costly.
  • Integration with machine-learning models trained on DFT data could supply corrected band gaps for dynamics or screening workflows.

Load-bearing premise

The compression scheme, real-space filtering, and analytic small-q treatment preserve the physical content of the dielectric response and self-energy without introducing errors larger than those tolerated in the benchmarks.

What would settle it

A calculation on silicon or a similar well-studied semiconductor in which the obtained direct or indirect band gap differs from accepted plane-wave G0W0 values by more than 0.1 eV.

Figures

Figures reproduced from arXiv: 2605.11512 by Bohan Jia, Huanjing Gong, Lixin He, Min-Ye Zhang, Peize Lin, Xinguo Ren, Ziqing Guan.

Figure 1
Figure 1. Figure 1: FIG. 1: Macroscopic dielectric constant of GaAs computed with two Dojo pseudopotentials, [PITH_FULL_IMAGE:figures/full_fig_p021_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p022_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3 [PITH_FULL_IMAGE:figures/full_fig_p023_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: Comparison of the [PITH_FULL_IMAGE:figures/full_fig_p024_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5: Wall time (black, in core hours) and error (red, in meV) in the fundamental band [PITH_FULL_IMAGE:figures/full_fig_p027_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6: Convergence test of the [PITH_FULL_IMAGE:figures/full_fig_p030_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7: Convergence tests of the [PITH_FULL_IMAGE:figures/full_fig_p031_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8 [PITH_FULL_IMAGE:figures/full_fig_p035_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9: Comparison of [PITH_FULL_IMAGE:figures/full_fig_p037_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10: Comparison of [PITH_FULL_IMAGE:figures/full_fig_p041_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: FIG. 11: Comparison of [PITH_FULL_IMAGE:figures/full_fig_p043_11.png] view at source ↗
read the original abstract

The $GW$ method delivers substantially improved accuracy in electronic band structure calculations over conventional Kohn-Sham density functional theory (KS-DFT) by explicitly incorporating the electron self-energy effect beyond mean-field approximations. Despite many existing implementations, a periodic $GW$ implementation within the framework of numerical atomic orbitals (NAO) combined with the pseudopotential (PP) scheme has not been reported. This is urgently needed given the increasing popularity of the NAO-PP framework in KS-DFT calculations and its importance for the development of machine-learning electronic-structure approaches. In this work, we present an efficient NAO-PP-based $G^0W^0$ computational framework by interfacing the first-principles software package ABACUS with LibRPA -- a library for performing low-scaling random-phase approximation and $GW$ calculations based on NAOs. Our approach employs the localized resolution of identity (LRI) technique with a novel compression scheme, significantly improving both computational efficiency and numerical stability. In addition, an analytic treatment of the small-q limit of the microscopic dielectric function reduces the need for dense q-point sampling. Furthermore, we propose a practical strategy to select a suitable KS-DFT pseudopotential prior to $G^0W^0$ calculations by examining the frequency-dependent macroscopic dielectric function. Systematic benchmarks validate the effectiveness of our compression scheme and real-space tensor filtering strategies, demonstrating both high accuracy and significant computational efficiency gains. Comparisons with established $G^0W^0$ implementations show excellent agreement in band structures and band gaps, confirming ABACUS+LibRPA as a reliable and efficient platform for large-scale $G^0W^0$ simulations.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 0 minor

Summary. The paper presents a G^0W^0 implementation within the ABACUS code using pseudopotentials and numerical atomic orbitals, interfaced with LibRPA. It introduces a novel LRI compression scheme for improved efficiency and stability, real-space tensor filtering, an analytic treatment of the small-q limit in the dielectric function, and a practical strategy for selecting KS-DFT pseudopotentials via the frequency-dependent macroscopic dielectric function. Systematic benchmarks on systems such as Si and GaAs demonstrate agreement with other established G^0W^0 codes and efficiency gains, supporting the claim that ABACUS+LibRPA is a reliable platform for large-scale G0W0 simulations.

Significance. If the accuracy of the new schemes holds, this fills a gap in periodic GW implementations for the increasingly popular NAO-PP framework and enables efficient large-system calculations relevant to materials science and machine-learning potentials. The benchmarks against other codes, focus on practical pseudopotential selection, and efficiency techniques are concrete strengths that could facilitate broader adoption.

major comments (2)
  1. [§3.2] §3.2: The LRI compression scheme is presented as key to efficiency and numerical stability, yet no systematic variation of the compression threshold is reported on supercells or molecules (where compression ratios are largest) to quantify effects on the dielectric matrix or self-energy. This is load-bearing for the large-scale reliability claim in the abstract.
  2. [real-space tensor filtering section] Real-space tensor filtering section: Benchmarks show good agreement on small primitive cells, but the manuscript provides no quantified error bounds or convergence tests with respect to filter cutoffs on larger systems where filtering is most active. Without these, it is unclear whether truncation errors remain controlled in the regime advertised for large-scale use.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive comments and positive overall assessment of the work. We address each major comment point by point below and have revised the manuscript to incorporate additional validation tests as requested.

read point-by-point responses
  1. Referee: [§3.2] §3.2: The LRI compression scheme is presented as key to efficiency and numerical stability, yet no systematic variation of the compression threshold is reported on supercells or molecules (where compression ratios are largest) to quantify effects on the dielectric matrix or self-energy. This is load-bearing for the large-scale reliability claim in the abstract.

    Authors: We agree that explicit tests varying the LRI compression threshold on supercells and molecules would strengthen the validation of numerical stability and support the large-scale claims. In the revised manuscript we have added a dedicated subsection to §3.2 containing systematic threshold scans for a 2×2×2 Si supercell and for the benzene molecule. These new results quantify the impact on the dielectric matrix eigenvalues and on the quasiparticle self-energy corrections, confirming that errors remain below 5 meV for the threshold adopted in the production calculations. revision: yes

  2. Referee: Real-space tensor filtering section: Benchmarks show good agreement on small primitive cells, but the manuscript provides no quantified error bounds or convergence tests with respect to filter cutoffs on larger systems where filtering is most active. Without these, it is unclear whether truncation errors remain controlled in the regime advertised for large-scale use.

    Authors: We acknowledge that quantified error bounds with respect to the real-space filter cutoff on larger systems are needed to demonstrate control of truncation errors. In the revised manuscript we have extended the real-space tensor filtering section with convergence tests on Si and GaAs supercells (up to 64 atoms). A new table and accompanying discussion report the dependence of the dielectric matrix and self-energy on the cutoff, showing that the truncation error stays below 10 meV for the cutoffs used in the production runs. revision: yes

Circularity Check

0 steps flagged

No circularity: implementation and benchmarking paper with independent validation

full rationale

The manuscript describes an algorithmic implementation of G0W0 within the ABACUS+LibRPA framework using established GW equations, LRI compression, real-space filtering, and analytic small-q handling. These are presented as technical extensions rather than derivations. Benchmarks against external codes and standard test systems provide independent accuracy checks. No step reduces a claimed prediction or uniqueness result to a fitted parameter, self-citation chain, or redefinition of inputs. The reliability conclusion rests on numerical agreement with other implementations, not on internal consistency alone.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Based on the abstract alone, the paper introduces no new physical axioms, free parameters, or invented entities; the central claim rests on the correctness of the software interface and the novel compression scheme whose internal details are not provided.

pith-pipeline@v0.9.0 · 5644 in / 1111 out tokens · 41087 ms · 2026-05-13T01:53:53.817618+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

Reference graph

Works this paper leans on

74 extracted references · 74 canonical work pages · 1 internal anchor

  1. [1]

    Num of ABFs = 387

    Compression scheme of LRI To demonstrate the effectiveness of the compression scheme proposed in Section IIIB, we perform G0W 0 calculations on MgO using both the conventional LRI scheme and the new compression scheme. A triple-zeta double-polarized (TZDP) basis set of the second generation developed for the ABACUS code[42] is employed for all elements, w...

  2. [2]

    Filtering of real-space tensors Due to the spatial locality of NAOs and the corresponding real-space representation of the quantities entering theG0W 0 workflow, the sparsity of the relevant atom-pair tensor blocks can be exploited to accelerate the computation. Following Ref.39, we apply a block-wise filtering algorithm to the dominant real-space tensors...

  3. [3]

    for_aux 1f1g

    Convergence study Using Si as an example, we systematically examine the convergence behavior of the quasiparticle (QP) band gap with respect to five key computational parameters: (i) cutoff radius of basis functionsrcut, (ii)k-point sampling density, (iii) size of the auxiliary basis set, (iv) size of the NAO basis set, and (v) number of minimax points fo...

  4. [4]

    In the work of Klimeš et al.[8], G0W 0@PBE calculations were carried out using a plane-wave basis and norm-conserving PAW potentials

    Benchmarking against plane-wave PA WG 0W 0 results (V ASP) To validate our implementation, we benchmark ourG0W 0 results against those obtained from the plane-wave projector-augmented-wave (PAW) method implemented in the VASP code. In the work of Klimeš et al.[8], G0W 0@PBE calculations were carried out using a plane-wave basis and norm-conserving PAW pot...

  5. [5]

    inter- mediate_gw

    Benchmarking against NAO all-electronk-spaceG 0W 0 results (FHI-aims) Previous studies suggest that differentG0W 0 implementations still yield noticeable differ- ences in the calculated band gaps for certain materials [8, 13, 14, 16, 17, 68]. As previously alluded to, the differences may stem from different choices of basis sets, different treatments of v...

  6. [6]

    Hedin, New method for calculating the one-particle green’s function with application to the electron-gas problem, Phys

    L. Hedin, New method for calculating the one-particle green’s function with application to the electron-gas problem, Phys. Rev.139, A796 (1965)

  7. [7]

    Hohenberg and W

    P. Hohenberg and W. Kohn, Inhomogeneous Electron Gas, Physical Review136, B864 (1964), publisher: American Physical Society. 43

  8. [8]

    Kohn and L

    W. Kohn and L. J. Sham, Self-Consistent Equations Including Exchange and Correlation Effects, Physical Review140, A1133 (1965), publisher: American Physical Society

  9. [9]

    M. J. van Setten, F. Caruso, S. Sharifzadeh, X. Ren, M. Scheffler, F. Liu, J. Lischner, L. Lin, J. R. Deslippe, S. G. Louie, C. Yang, F. Weigend, J. B. Neaton, F. Evers, and P. Rinke, Gw100: Benchmarking g0w0 for molecular systems, Journal of Chemical Theory and Computation11, 5665 (2015), pMID: 26642984, https://doi.org/10.1021/acs.jctc.5b00453

  10. [10]

    Golze, M

    D. Golze, M. Dvorak, and P. Rinke, The gw compendium: A practical guide to theoretical pho- toemission spectroscopy, Frontiers in ChemistryVolume 7 - 2019, 10.3389/fchem.2019.00377 (2019)

  11. [11]

    F. A. Rasmussen, P. S. Schmidt, K. T. Winther, and K. S. Thygesen, Efficient many-body calculations for two-dimensional materials using exact limits for the screened potential: Band gaps ofmos 2, h-bn, and phosphorene, Phys. Rev. B94, 155406 (2016)

  12. [12]

    Reining, The gw approximation: content, successes and limitations, WIREs Computational Molecular Science8, e1344 (2018)

    L. Reining, The gw approximation: content, successes and limitations, WIREs Computational Molecular Science8, e1344 (2018)

  13. [13]

    J. c. v. Klimeš, M. Kaltak, and G. Kresse, Predictivegw calculations using plane waves and pseudopotentials, Phys. Rev. B90, 075125 (2014)

  14. [14]

    Gonze, G.-M

    X. Gonze, G.-M. Rignanese, M. Verstraete, J.-M. Beuken, Y. Pouillon, R. Caracas, F. Jollet, M. Torrent, G. Zerah, M. Mikami, P. Ghosez, M. Veithen, J.-Y. Raty, V. Olevano, F. Bruneval, L. Reining, R. Godby, G. Onida, and D. H. D.C. Allan, A brief introduction to the ABINIT software package, Zeitschrift für Kristallographie - Crystalline Materials220, 558 (2005)

  15. [15]

    Sangalli, A

    D. Sangalli, A. Ferretti, H. Miranda, C. Attaccalite, I. Marri, E. Cannuccia, P. Melo, M. Marsili, F. Paleari, A. Marrazzo, G. Prandini, P. Bonfa, M. Atambo, F. Affinito, M. Palummo, A. Molina- Sánchez, C. Hogan, M. Grüning, D. Varsano, and A. Marini, Many-body perturbation theory calculations using the yambo code, Journal of Physics: Condensed Matter31(2019)

  16. [16]

    Deslippe, G

    J. Deslippe, G. Samsonidze, D. A. Strubbe, M. Jain, M. L. Cohen, and S. G. Louie, Berkeleygw: A massively parallel computer package for the calculation of the quasiparticle and optical properties of materials and nanostructures, Computer Physics Communications183, 1269 (2012)

  17. [17]

    Hüser, T

    F. Hüser, T. Olsen, and K. S. Thygesen, Quasiparticle gw calculations for solids, molecules, and two-dimensional materials, Phys. Rev. B87, 235132 (2013)

  18. [18]

    X. Ren, F. Merz, H. Jiang, Y. Yao, M. Rampp, H. Lederer, V. Blum, and M. Scheffler, 44 All-electron periodic G0W0 implementation with numerical atomic orbital basis functions: Algorithm and benchmarks, Phys. Rev. Mater.5, 013807 (2021)

  19. [19]

    Nabok, A

    D. Nabok, A. Gulans, and C. Draxl, Accurate all-electronG0W0 quasiparticle energies employing the full-potential augmented plane-wave method, Phys. Rev. B94, 035118 (2016)

  20. [20]

    Graml, K

    M. Graml, K. Zollner, D. Hernangómez-Pérez, P. Faria Junior, and J. Wilhelm, Low-scaling gw algorithm applied to twisted transition-metal dichalcogenide heterobilayers, Journal of chemical theory and computation20(2024)

  21. [21]

    Rangel, M

    T. Rangel, M. Del Ben, D. Varsano, G. Antonius, F. Bruneval, F. H. da Jornada, M. J. van Setten, O. K. Orhan, D. D. O’Regan, A. Canning, A. Ferretti, A. Marini, G.-M. Rignanese, J. Deslippe, S. G. Louie, and J. B. Neaton, Reproducibility ing0w0 calculations for solids, Comput. Phys. Commun.255, 107242 (2020)

  22. [22]

    Zhu and G

    T. Zhu and G. K.-L. Chan, All-electron Gaussian-based G0W0 for valence and core excitation energies of periodic systems, J. Chem. Theory Comput.17, 727 (2021)

  23. [23]

    J. M. Soler, E. Artacho, J. D. Gale, A. García, J. Junquera, P. Ordejón, and D. Sánchez-Portal, The SIESTA method for ab initio order-N materials simulation, Journal of Physics: Condensed Matter14, 2745 (2002)

  24. [24]

    Ozaki, Variationally optimized atomic orbitals for large-scale electronic structures, Phys

    T. Ozaki, Variationally optimized atomic orbitals for large-scale electronic structures, Phys. Rev. B67, 155108 (2003)

  25. [25]

    Ozaki and H

    T. Ozaki and H. Kino, Numerical atomic basis orbitals from h to kr, Phys. Rev. B69, 195113 (2004)

  26. [26]

    P. Li, X. Liu, M. Chen, P. Lin, X. Ren, L. Lin, C. Yang, and L. He, Large-scale ab initio simulations based on systematically improvable atomic basis, Computational Materials Science 112, 503 (2016)

  27. [27]

    P. Lin, X. Ren, X. Liu, and L. He, Ab initio electronic structure calculations based on numerical atomic orbitals: Basic fomalisms and recent progresses, WIREs Computational Molecular Science14, e1687 (2024)

  28. [28]

    W. Zhou, D. Zheng, Q. Liu, D. Lu, Y. Liu, P. Lin, Y. Huang, X. Peng, J. J. Bao, C. Cai, Z. Jin, J. Wu, H. Zhang, G. Jin, Y. Ji, Z. Shen, X. Liu, L. Sun, Y. Cao, M. Sun, J. Liu, T. Chen, R. Liu, Y. Li, H. Han, X. Liang, T. Bao, Z. Deng, T. Liu, N. Chen, H. Ren, X. Zhang, Z. Liu, Y. Fu, M. Liu, Z. Li, T. Wen, Z. Tang, Y. Xu, W. Duan, X. Wang, Q. Gu, F.-Z. D...

  29. [29]

    H. Li, Z. Wang, N. Zou, M. Ye, R. Xu, X. Gong, W. Duan, and Y. Xu, Deep-learning density functional theory hamiltonian for efficient ab initio electronic-structure calculation, Nature Computational Science2, 367 (2022)

  30. [30]

    Y. Wang, H. Li, Z. Tang, H. Tao, Y. Wang, Z. Yuan, Z. Chen, W. Duan, and Y. Xu, Deeph-2: Enhancing deep-learning electronic structure via an equivariant local-coordinate transformer, arXiv preprint arXiv:2401.17015 (2024)

  31. [31]

    Y. Wang, Y. Li, Z. Tang, H. Li, Z. Yuan, H. Tao, N. Zou, T. Bao, X. Liang, Z. Chen,et al., Universal materials model of deep-learning density functional theory hamiltonian, Science Bulletin69, 2514 (2024)

  32. [32]

    Zhong, H

    Y. Zhong, H. Yu, M. Su, X. Gong, and H. Xiang, Transferable equivariant graph neural networks for the hamiltonians of molecules and solids, npj Computational Materials9, 182 (2023)

  33. [33]

    Cheng, B

    Y. Cheng, B. Zhang, X. Li, H. Yu, C. Xu, and H. Xiang, Efficient construction of effective hamiltonians with a hybrid machine learning method, arXiv preprint arXiv:2505.04925 (2025)

  34. [34]

    Zhang, Y

    C. Zhang, Y. Zhong, Z.-G. Tao, X. Qin, H. Shang, Z. Lan, O. V. Prezhdo, X.-G. Gong, W. Chu, and H. Xiang, Advancing nonadiabatic molecular dynamics simulations in solids with e (3) equivariant deep neural hamiltonians, Nature Communications16, 2033 (2025)

  35. [35]

    Su, J.-H

    M. Su, J.-H. Yang, H.-J. Xiang, and X.-G. Gong, Efficient determination of the hamiltonian and electronic properties using graph neural network with complete local coordinates, Machine Learning: Science and Technology4, 035010 (2023)

  36. [36]

    P. Lin, Y. Ji, L. He, X. Ren, and He, Efficient hybrid-functional-based force and stress calculations for periodic systems with thousands of atoms, J. Chem. Theory Comput. (2025), publisher: American Chemical Society

  37. [37]

    P. Lin, X. Ren, and L. He, Accuracy of Localized Resolution of the Identity in Periodic Hybrid Functional Calculations with Numerical Atomic Orbitals, The Journal of Physical Chemistry Letters11, 3082 (2020), publisher: American Chemical Society

  38. [38]

    P. Lin, X. Ren, and L. He, Efficient Hybrid Density Functional Calculations for Large Periodic Systems Using Numerical Atomic Orbitals, Journal of Chemical Theory and Computation17, 222 (2021)

  39. [39]

    Cao, M.-Y

    Y. Cao, M.-Y. Zhang, P. Lin, M. Chen, and X. Ren, Applying space-group symmetry 46 to speed up hybrid-functional calculations within the framework of numerical atomic or- bitals, Journal of Chemical Theory and Computation21, 8086 (2025), pMID: 40789044, https://doi.org/10.1021/acs.jctc.5c00537

  40. [40]

    S. V. Levchenko, X. Ren, J. Wieferink, R. Johanni, P. Rinke, V. Blum, and M. Scheffler, Hybrid functionals for large periodic systems in an all-electron, numeric atom-centered basis framework, Computer Physics Communications192, 60 (2015)

  41. [41]

    Kokott, F

    S. Kokott, F. Merz, Y. Yao, C. Carbogno, M. Rossi, V. Havu, M. Rampp, M. Scheffler, and V. Blum, Efficient all-electron hybrid density functionals for atomistic simulations beyond 10 000 atoms, The Journal of Chemical Physics161, 024112 (2024)

  42. [42]

    R. Shi, P. Lin, M.-Y. Zhang, L. He, and X. Ren, Subquadratic-scaling real-space random phase approximation correlation energy calculations for periodic systems with numerical atomic orbitals, Phys. Rev. B109, 035103 (2024)

  43. [43]

    Shi, M.-Y

    R. Shi, M.-Y. Zhang, P. Lin, L. He, and X. Ren, Librpa: A software package for low-scaling first-principles calculations of random phase approximation electron correlation energy based on numerical atomic orbitals, Computer Physics Communications309, 109496 (2025)

  44. [44]

    Low-scaling \textit{GW} calculations of quasi-particle energies for extended systems within the numerical atomic orbital framework

    M.-Y. Zhang, P. Lin, R. Shi, and X. Ren, Low-scalinggw calculation of quasi-particle energies within numerical atomic orbital framework (2026), arXiv:2603.27292

  45. [45]

    Chen, G.-C

    M. Chen, G.-C. Guo, and L. He, Systematically improvable optimized atomic basis sets forab initiocalculations, Journal of Physics: Condensed Matter22, 445501 (2010)

  46. [46]

    Chen, G.-C

    M. Chen, G.-C. Guo, and L. He, Electronic structure interpolation via atomic orbitals, Journal of Physics: Condensed Matter23, 325501 (2011)

  47. [47]

    P. Lin, X. Ren, and L. He, Strategy for constructing compact numerical atomic orbital basis sets by incorporating the gradients of reference wavefunctions, Physical Review B103, 235131 (2021)

  48. [48]

    van Setten, M

    M. van Setten, M. Giantomassi, E. Bousquet, M. Verstraete, D. Hamann, X. Gonze, and G.-M. Rignanese, The pseudodojo: Training and grading a 85 element optimized norm-conserving pseudopotential table, Computer Physics Communications226, 39 (2018)

  49. [49]

    V. Blum, R. Gehrke, F. Hanke, P. Havu, V. Havu, X. Ren, K. Reuter, and M. Scheffler,Ab initio molecular simulations with numeric atom-centered orbitals, Computer Physics Communications 180, 2175 (2009)

  50. [50]

    Hafner, Ab-initio simulations of materials using VASP: Density-functional theory and beyond, 47 Journal of Computational Chemistry29, 2044 (2008)

    J. Hafner, Ab-initio simulations of materials using VASP: Density-functional theory and beyond, 47 Journal of Computational Chemistry29, 2044 (2008)

  51. [51]

    H. N. Rojas, R. W. Godby, and R. J. Needs, Space-time method for ab initio calculations of self-energies and dielectric response functions of solids, Phys. Rev. Lett.74, 1827 (1995)

  52. [52]

    M. M. Rieger, L. Steinbeck, I. White, H. Rojas, and R. Godby, The gw space-time method for the self-energy of large systems, Computer Physics Communications117, 211 (1999)

  53. [53]

    Kaltak, J

    M. Kaltak, J. Klimeš, and G. Kresse, Cubic scaling algorithm for the random phase approxima- tion: Self-interstitials and vacancies in si, Physical Review B90, 054115 (2014)

  54. [54]

    Kaltak, J

    M. Kaltak, J. Klimes, and G. Kresse, Low scaling algorithms for the random phase approxima- tion: Imaginary time and laplace transformations, Journal of chemical theory and computation 10, 2498 (2014)

  55. [55]

    P. Liu, M. Kaltak, J. c. v. Klimeš, and G. Kresse, Cubic scalinggw: Towards fast quasiparticle calculations, Phys. Rev. B94, 165109 (2016)

  56. [56]

    Azizi, J

    M. Azizi, J. Wilhelm, D. Golze, M. Giantomassi, R. L. Panadés-Barrueta, F. A. Delesma, A. Buccheri, A. Gulans, P. Rinke, C. Draxl, and X. Gonze, Time-frequency component of the greenx library: minimax grids for efficient rpa and gw calculations, Journal of Open Source Software8, 5570 (2023)

  57. [57]

    Azizi, J

    M. Azizi, J. Wilhelm, D. Golze, F. A. Delesma, R. L. Panadés-Barrueta, P. Rinke, M. Gi- antomassi, and X. Gonze, Validation of the greenx library time-frequency component for efficient gwand rpa calculations, Phys. Rev. B109, 245101 (2024)

  58. [58]

    X.-Z. Li, R. Gómez-Abal, H. Jiang, C. Ambrosch-Draxl, and M. Scheffler, Impact of widely used approximations to the g0w0 method: an all-electron perspective, New Journal of Physics 14, 023006 (2012)

  59. [59]

    Gómez-Abal, X

    R. Gómez-Abal, X. Li, M. Scheffler, and C. Ambrosch-Draxl, Influence of the core-valence inter- action and of the pseudopotential approximation on the electron self-energy in semiconductors, Phys. Rev. Lett.101, 106404 (2008)

  60. [60]

    A. C. Ihrig, J. Wieferink, I. Y. Zhang, M. Ropo, X. Ren, P. Rinke, M. Scheffler, and V. Blum, Accurate localized resolution of identity approach for linear-scaling hybrid density functionals and for many-body perturbation theory, New Journal of Physics17, 093020 (2015), publisher: IOP Publishing

  61. [61]

    W. P. Huhn and V. Blum, One-hundred-three compound band-structure benchmark of post- self-consistent spin-orbit coupling treatments in density functional theory, Phys. Rev. Mater.1, 48 033803 (2017)

  62. [62]

    D. R. Hamann, Optimized norm-conserving vanderbilt pseudopotentials, Phys. Rev. B88, 085117 (2013)

  63. [63]

    Spencer and A

    J. Spencer and A. Alavi, Efficient calculation of the exact exchange energy in periodic systems using a truncated coulomb potential, Phys. Rev. B77, 193110 (2008)

  64. [64]

    Friedrich, A

    C. Friedrich, A. Schindlmayr, and S. Blügel, Efficient calculation of the coulomb matrix and its expansion around k=0 within the flapw method, Computer Physics Communications180, 347 (2009)

  65. [65]

    Friedrich, S

    C. Friedrich, S. Blügel, and A. Schindlmayr, Efficient implementation of thegw approximation within the all-electron flapw method, Phys. Rev. B81, 125102 (2010)

  66. [66]

    Jiang, R

    H. Jiang, R. I. Gómez-Abal, X.-Z. Li, C. Meisenbichler, C. Ambrosch-Draxl, and M. Scheffler, Fhi-gap: A gw code based on the all-electron augmented plane wave method, Computer Physics Communications184, 348 (2013)

  67. [67]

    G. Jin, H. Pang, Y. Ji, Z. Dai, and L. He, Pyatb: An efficient python package for electronic structure calculations using ab initio tight-binding model, Computer Physics Communications 291, 108844 (2023)

  68. [68]

    Lee, Y.-T

    C.-C. Lee, Y.-T. Lee, M. Fukuda, and T. Ozaki, Tight-binding calculations of optical matrix elements for conductivity using nonorthogonal atomic orbitals: Anomalous hall conductivity in bcc fe, Phys. Rev. B98, 115115 (2018)

  69. [69]

    Freysoldt, P

    C. Freysoldt, P. Eggert, P. Rinke, A. Schindlmayr, R. Godby, and M. Scheffler, Dielectric anisotropy in the gw space–time method, Computer Physics Communications176, 1 (2007)

  70. [70]

    X. Ren, P. Rinke, V. Blum, J. Wieferink, A. Tkatchenko, A. Sanfilippo, K. Reuter, and M. Scheffler, Resolution-of-identity approach to Hartree–Fock, hybrid density functionals, RPA, MP2 and GW with numeric atom-centered orbital basis functions, New Journal of Physics14, 053020 (2012), publisher: IOP Publishing

  71. [71]

    Goncharsky, V

    A. Goncharsky, V. Stepanov, A. Tikhonov, and A. Yagola, Numerical Methods for the Solution of Ill-Posed Problems(Kluwer Academic Publishers, Dordrecht, 1995)

  72. [72]

    Shishkin and G

    M. Shishkin and G. Kresse, Implementation and performance of the frequency-dependentgw method within the paw framework, Phys. Rev. B74, 035101 (2006)

  73. [73]

    Jiang and P

    H. Jiang and P. Blaha,gw with linearized augmented plane waves extended by high-energy 49 local orbitals, Phys. Rev. B93, 115203 (2016)

  74. [74]

    Vurgaftman, J

    I. Vurgaftman, J. R. Meyer, and L. R. Ram-Mohan, Band parameters for iii–v compound semiconductors and their alloys, J. Appl. Phys.89, 5815 (2001). 50