Scientific Calendar Event



Starts 15 Dec 2021 11:00
Ends 15 Dec 2021 12:00
Central European Time
Virtual

Iurii Timrov
(THEOS and MARVEL, EPFL, Lausanne, Switzerland)


Density-functional theory (DFT) with extended Hubbard functionals is a powerful method for studying complex materials containing transition-metal and rare-earth elements, owing to its accuracy in correcting self-interactions and its low computational costs [1]. There are two key elements in these formulations which are closely interconnected: i) the choice of the on-site U and inter-site V Hubbard parameters, and ii) the choice of the Hubbard manifold. Recently, we developed an automated and reliable approach for the first-principles determination of U and V using density-functional perturbation theory (DFPT) [2,3]. In this talk I will show that DFPT allows us to reduce significantly computational costs, improve numerical accuracy, and fully automate the calculation of the Hubbard parameters by recasting the linear response of a localized perturbation in supercells into an array of monochromatic perturbations that can be calculated in the primitive cell. This framework can be used with different Hubbard manifolds, such as nonorthogonalized and orthogonalized atomic orbitals, including the respective calculation of Pulay (Hubbard) forces and stresses [4] that are needed for the self-consistent evaluation of Hubbard parameters [3]. I will show how this formalism can be used for the evaluation of such properties as voltages in Li-ion batteries, formation energies of oxygen vacancies in perovskites, and I will discuss the applicability of this formalism for improving band gaps with respect to standard DFT [5] and its use for searching of novel materials for the photocatalytic water splitting [6].  Finally, I will present the extension of this framework to the calculations of phonons [7] and electron-phonon coupling [8] in selected transition-metal compounds. These tools are implemented in the open-source Quantum ESPRESSO distribution [9] and are available to the community at large.


[1] V.L. Campo Jr and M. Cococcioni, J. Phys.: Condens. Matter. 22, 055602 (2010).
[2] I. Timrov, N. Marzari, M. Cococcioni, Phys. Rev. B 98, 085127 (2018).
[3] I. Timrov, N. Marzari, M. Cococcioni, Phys. Rev. B 103, 045141 (2021).
[4] I. Timrov, F. Aquilante, L. Binci, M. Cococcioni, N. Marzari, Phys. Rev. B 102, 235159 (2020).
[5] N.E. Kirchner-Hall, W. Zhao, Y. Xiong, I. Timrov, I. Dabo, Appl, Sci. 11, 2395 (2021).
[6] Y. Xiong et al., Energy Environ. Sci. 14, 2335 (2021).
[7] A. Floris, I. Timrov, B. Himmetoglu, N. Marzari, S. de Gironcoli, M. Cococcioni, Phys. Rev. B 101, 064305 (2020).
[8] J.-J. Zhou, J. Park, I. Timrov, A. Floris, M. Cococcioni, N. Marzari, M. Bernardi, Phys. Rev. Lett. 127, 126404 (2021).
[9] P. Giannozzi et al., J. Phys.: Condens. Matter 29, 465901 (2017).



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