2013
DOI: 10.1103/physrevb.87.241101
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Formation of orbital-selective electron states in LaTiO3/SrTiO3superlattices

Abstract: The interface electronic structure of correlated LaTiO 3 /SrTiO 3 superlattices is investigated by means of the charge self-consistent combination of the local density approximation (LDA) to density functional theory with dynamical mean-field theory. Utilizing a pseudopotential technique together with a continuous-time quantum Monte Carlo approach, the resulting complex multiorbital electronic states are addressed in a coherent fashion beyond static mean field. General structural relaxations are taken into acc… Show more

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Cited by 17 publications
(25 citation statements)
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“…But since our focus is on the challenging large-scale heterostructure problem, where such recent extensions are very expensive, we work in a minimal t g 2 -based correlation framework. In an initial study [10], the δ-doping of LTO with a single SrO layer was in part already investigated within DFT+DMFT. But there the inplane lattice constant a = b of bulk SrTiO 3 , a site-averaged DC as well as cubic t g 2 projections (i.e., not adapted to the local cf eigenbasis) were used.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
See 1 more Smart Citation
“…But since our focus is on the challenging large-scale heterostructure problem, where such recent extensions are very expensive, we work in a minimal t g 2 -based correlation framework. In an initial study [10], the δ-doping of LTO with a single SrO layer was in part already investigated within DFT+DMFT. But there the inplane lattice constant a = b of bulk SrTiO 3 , a site-averaged DC as well as cubic t g 2 projections (i.e., not adapted to the local cf eigenbasis) were used.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
“…As a specific realization thereof, the δ-doped oxide heterostructures [4][5][6][7] (i.e., introducing well-defined impurity monolayers into a given host oxide compound) recently emerged as a canonical method to create challenging electronic states from experimental fabrication. Especially, the δ-doping of Mott insulators [8][9][10][11] not only has relevance in the designing context, but furthermore sheds light on the generic physics of the realistic doped-Mott state in a controlled way without the usual complications arising from disorder and other features of random impurity doping.…”
Section: Introductionmentioning
confidence: 99%
“…While STO is an ideal cubic perovskite at ambient temperature, LTO marks a distorted perovskite with orthorhombic crystal symmetry. (Lechermann et al 2013)). Left: total spectrum, right: closer to Fermi level.…”
Section: Mott-band Insulator Architecturesmentioning
confidence: 99%
“…For an electron the charge e q e = − and for a hole h q e = + and V is the potential energy associated with the band width. A restrictive presumption is the wavelength much larger than the lattice constant at which the nonstationary electric field E = −A  is regarded as spatially homogeneous and the terms 2 …”
Section: Lagrange-hamilton Approach For Electron-hole Pairmentioning
confidence: 99%
“…In these strongly correlated materials interactions between the charged particles play a major role in determining optical and transport properties: each single particle has a complex influence on its neighbors and interacts with both antiparticles (electrons-holes) as well as with crystalline phonons. The elaborated models based on the density functional theory (DFT) and the dynamical mean-field theory of strongly correlated fermion systems (DMFT) which now became the standard for fermionic correlation problems [1][2][3]. Nevertheless, the uncertainty in the choice of model parameters prevent the DFT+DMFT approaches from being flexible enough to capture entirely the quantum many-body problem of realistic complexity.…”
Section: Introductionmentioning
confidence: 99%