2018
DOI: 10.1103/physrevmaterials.2.085801
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Diffusion Monte Carlo: A pathway towards an accurate theoretical description of manganese oxides

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Cited by 18 publications
(26 citation statements)
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References 119 publications
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“…This agrees very well with the photoluminescence and UV/Vis [125,126] experiments and also with PBE0, where a band gap of 3.2-3.3 eV is obtained using QE-RRKJ and CRYSTAL-LCAO. DMC band gaps are larger than the hybrid-DFT band gaps as observed previously [32,46,87]. We used a simple single-determinant scheme to obtain the band gaps from DMC; therefore, our results should be treated as an upper bound due to the fixed node bias, which may not fully cancel between the ground and excited states.…”
Section: Electronic Structure Quasiparticle and Optical Gapsmentioning
confidence: 78%
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“…This agrees very well with the photoluminescence and UV/Vis [125,126] experiments and also with PBE0, where a band gap of 3.2-3.3 eV is obtained using QE-RRKJ and CRYSTAL-LCAO. DMC band gaps are larger than the hybrid-DFT band gaps as observed previously [32,46,87]. We used a simple single-determinant scheme to obtain the band gaps from DMC; therefore, our results should be treated as an upper bound due to the fixed node bias, which may not fully cancel between the ground and excited states.…”
Section: Electronic Structure Quasiparticle and Optical Gapsmentioning
confidence: 78%
“…However, the accuracy of DFT has not yet been sufficient to differentiate between the two mechanisms [4,7]. Projector methods [24], such as Diffusion Monte Carlo (DMC) [25,26], are shown to be the most accurate and practical methods to tackle the ground states of complex, highly correlated materials with a similar success in the excited states [27][28][29][30][31][32][33][34][35][36][37][38][39][40][41][42][43]. Although it is computationally more expensive, DMC explicitly accounts for the antisymmetry of the many-body wave function and electron correlation, without using any empirical parameters [25,26,44,45].…”
Section: Introductionmentioning
confidence: 99%
“…1(b for the actual structure), whose total energy is estimated as E tot (chain) = −33.99 eV. Thus, the total energies of the two structures turn out to be quite close to each other; considering the accuracy of the first principles calculation, a difference of 40 meV can be reversed, e.g., by the effects of the correlation and/or excess oxygens not taken into account here [55]. Then, given the fact that the chain-type structure is known to be realized in an existing material Sr 2 CuO 3 [18][19][20] but inconsistent with the tetragonal symmetry, the Lieb-latticetype structure may be considered as a realistic candidate for the lattice structure of Ba 2 CuO 3+δ .…”
Section: A Stability Of the Lieb Structure For Ba 2 Cuomentioning
confidence: 82%
“…For Mn and O atoms, we used hard norm-conserving RRKJ (OPT) pseudopotentials 50 . These potentials have been thoroughly tested in previous DMC works for Mn and O-based materials 33,50 . For these pseudopotentials, we used a kinetic energy cutoff of 300 Ry.…”
Section: Methodsmentioning
confidence: 99%
“…This method has a weaker dependence on the starting Hubbard parameter and density functional and can successfully achieve results with an accuracy beyond the mean field approximation 19 . For example, DMC has succesfully been used to calculate the spin superexchange in the correlated cuprate Ca 2 CuO 3 31 , has been used to successfully predict the magnetic structure in FeSe when DFT methods disagreed 32 , and has been applied to bulk polymorphs of MnO 2 to achieve band gap and lattice constant values in excellent agreement with experiment 33 and has been applied to study the excitation energies of Mn 4+ doped phosphors 41 (both Mn-based studies used the same RRKJ pseudopotentials we used in our work 33,41 ).…”
Section: Introductionmentioning
confidence: 99%