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Hybridization-Switching Induced Mott Transition in ABO3 Perovskites

Atanu Paul, Anamitra Mukherjee, Indra Dasgupta, Arun Paramekanti, and Tanusri Saha-Dasgupta
Phys. Rev. Lett. 122, 016404 – Published 10 January 2019
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Abstract

We propose the concept of a “hybridization-switching induced Mott transition” which is relevant to a broad class of ABO3 perovskite materials including BiNiO3 and PbCrO3 that feature extended 6s orbitals on the A-site cation (Bi or Pb), and a strong AO covalency induced ligand hole. Using ab initio electronic structure and slave rotor theory calculations, we show that such systems exhibit a breathing phonon driven A-site to oxygen hybridization-wave instability which conspires with strong correlations on the B-site transition metal ion (Ni or Cr) to trigger a Mott insulating state. This class of systems is shown to undergo a pressure induced insulator to metal transition accompanied by a colossal volume collapse due to ligand hybridization switching.

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  • Received 25 January 2018
  • Revised 20 May 2018

DOI:https://doi.org/10.1103/PhysRevLett.122.016404

© 2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Atanu Paul1, Anamitra Mukherjee2, Indra Dasgupta1, Arun Paramekanti3, and Tanusri Saha-Dasgupta4,5,*

  • 1Department of Solid State Physics, Indian Association for the Cultivation of Science, Kolkata 700 032, India
  • 2School of Physical Sciences, National Institute of Science Education and Research, HBNI, Jatni 752050, India
  • 3Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7
  • 4Department of Condensed Matter Physics and Materials Science, S.N. Bose National Centre for Basic Sciences, Kolkata 700098, India
  • 5Center for Mathematical, Computational and Data Science, Indian Association for the Cultivation of Science, Kolkata 700 032, India

  • *t.sahadasgupta@gmail.com

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Issue

Vol. 122, Iss. 1 — 11 January 2019

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Images

  • Figure 1
    Figure 1

    (a) DFT cohesive energy versus volume for AP (triclinic) and HP (orthorhombic) BiNiO3; the intersection points of the plotted common tangent with the two curves yields the volume change ΔV/V3% at the transition. (b) Elastic energy of the NiO sublattice as a function of O-displacement for the HP (dashed) and AP (solid) volumes. Inset shows similar plot for the BiO sublattice.

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  • Figure 2
    Figure 2

    (a) GGA+U projected DOS of BiNiO3 in AP (top panels) and HP (bottom panels) phase. Left, middle, and right panels show projections to Bi-s (displaying relevant energy ranges), Ni-d, and O-p. Zero of energy is set at GGA+U Fermi energies. For AP, projections to Bi1 (solid, black) and Bi2 (shaded) are shown separately. (b) Calculated energy levels of Bi-s, O-p, and Ni-eg in the AP and HP phase. Zero of energy is set at Ni-eg.

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  • Figure 3
    Figure 3

    Phase diagram varying κ and εBεOx for (a) U/tB=6.5 and (b) U/tB=2.5. (c) DOS NTot(ω) for typical points in AP and HP phases, marked by stars in (a), as well as DOS for the metastable AP phase with imposed φ=0.

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  • Figure 4
    Figure 4

    Bond-dependent kinetic energy from the model (color bar shows magnitude) for BO and AO sublattices in the AP [(a) and (b)] and HP [(d) and (c)] phase, projected to the xy plane. Constant amplitude surfaces of DFT O-p Wannier functions for BiNiO3 at AP (e) and HP (f), superposed on NiO6 octahedra with adjacent two Bi ions. Cyan (light) and magenta (dark) colors indicate opposite signs.

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