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Electron-lattice interactions strongly renormalize the charge-transfer energy in the spin-chain cuprate Li2CuO2.


ABSTRACT: Strongly correlated insulators are broadly divided into two classes: Mott-Hubbard insulators, where the insulating gap is driven by the Coulomb repulsion U on the transition-metal cation, and charge-transfer insulators, where the gap is driven by the charge-transfer energy ? between the cation and the ligand anions. The relative magnitudes of U and ? determine which class a material belongs to, and subsequently the nature of its low-energy excitations. These energy scales are typically understood through the local chemistry of the active ions. Here we show that the situation is more complex in the low-dimensional charge-transfer insulator Li2CuO2, where ? has a large non-electronic component. Combining resonant inelastic X-ray scattering with detailed modelling, we determine how the elementary lattice, charge, spin and orbital excitations are entangled in this material. This results in a large lattice-driven renormalization of ?, which significantly reshapes the fundamental electronic properties of Li2CuO2.

SUBMITTER: Johnston S 

PROVIDER: S-EPMC4757783 | biostudies-literature | 2016 Feb

REPOSITORIES: biostudies-literature

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Electron-lattice interactions strongly renormalize the charge-transfer energy in the spin-chain cuprate Li2CuO2.

Johnston Steve S   Monney Claude C   Bisogni Valentina V   Zhou Ke-Jin KJ   Kraus Roberto R   Behr Günter G   Strocov Vladimir N VN   Málek Jiři J   Drechsler Stefan-Ludwig SL   Geck Jochen J   Schmitt Thorsten T   van den Brink Jeroen J  

Nature communications 20160217


Strongly correlated insulators are broadly divided into two classes: Mott-Hubbard insulators, where the insulating gap is driven by the Coulomb repulsion U on the transition-metal cation, and charge-transfer insulators, where the gap is driven by the charge-transfer energy Δ between the cation and the ligand anions. The relative magnitudes of U and Δ determine which class a material belongs to, and subsequently the nature of its low-energy excitations. These energy scales are typically understoo  ...[more]

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