2012
DOI: 10.1103/physrevlett.109.156402
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Site-Selective Mott Transition in Rare-Earth-Element Nickelates

Abstract: A combination of density functional and dynamical mean field theory calculations are used to show that the remarkable metal-insulator transition in the rare earth nickelate perovskites arise from a site-selective Mott phase, in which the d-electrons on a half of the Ni ions are localized to form a fluctuating moment while the d-electrons on other Ni ions form a singlet with holes on the surrounding oxygen ions. The calculation reproduces key features observed in the nickelate materials, including an insulating… Show more

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Cited by 300 publications
(345 citation statements)
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“…Though such a compromise exists, it seems to be unpopular, and strong opinions in favor of the ligand-hole picture are often voiced. 4 Going further, Sawatzky has proposed a picture for the observed "charge" ordering in terms of local Kondo screening of half the Ni 2+ spins 5 . A recent DMFT paper seems to suggest a similar scenario.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Though such a compromise exists, it seems to be unpopular, and strong opinions in favor of the ligand-hole picture are often voiced. 4 Going further, Sawatzky has proposed a picture for the observed "charge" ordering in terms of local Kondo screening of half the Ni 2+ spins 5 . A recent DMFT paper seems to suggest a similar scenario.…”
Section: Introductionmentioning
confidence: 99%
“…A recent DMFT paper seems to suggest a similar scenario. 4 A physical understanding of how such Kondo screening might come about, and whether it can account for the observed charge/spin order, is, however, still lacking.…”
Section: Introductionmentioning
confidence: 99%
“…13 This symmetry lowering has been associated with the occurrence of a breathing distortion of the oxygen octahedra, establishing two inequivalent nickel sites. [13][14][15][16] Finally, RE-NiO 3 (RNOs) undergo a paramagnetic (PM) to antiferromagnetic (AFM) transition at T = T Néel . The AFM structure gives rise to a magnetic diffraction peak with the Bragg vector q Bragg = ( 1 4 1 4 1 4 ), in pseudo-cubic (pc) notation.…”
mentioning
confidence: 99%
“…(9). By the comparison demonstrated in Figure 5, we emphasize that the two-particle approach based on vertex calculations in local DMFT is a convenient starting point to study the dynamics of spin fluctuations in correlated materials, given the availability of numerical packages 23,45 combining local DMFT and first principles methods, and their success in predicting the electronic structures of various correlated materials [46][47][48][49] .…”
Section: -9mentioning
confidence: 99%