Abstract

The electron–lattice interaction gives rise to a rich set of phenomena in quantum materials. Microscopically, this interaction often arises from the modulation of orbital overlaps; however, many theoretical studies neglect such couplings. Here, we present an exact diagonalization and determinant quantum Monte Carlo study of a three-orbital Su–Schrieffer–Heeger (SSH) model, on a two-dimensional Lieb lattice and in the negative charge transfer regime. At half-filling (one hole/unit cell), we observe a bipolaron insulating phase with a bond-disproportionate lattice. This phase is robust against moderate hole doping but is suppressed at large hole concentrations, leading to a metallic polaron-liquid-like state with fluctuating patches of local distortions. We also find an s-wave superconducting state at large hole doping that primarily appears on the oxygen sublattice. Our work provides a non-perturbative view of SSH-type couplings in two dimensions with implications for materials where such couplings are dominant.

Highlights

  • Lattice dimerization, referring to an alternation of two lattice constants, occurs in many quantum materials, including the organic charge-transfer solids[1,2,3], and perovskites systems like the rare-earth nickelates RNiO34–6, and the high-temperature superconducting bismuthates Bi1−xKxBiO3 (BKBO)[7,8]

  • Near half-filling, we find that the system is a bipolaronic charge-density-wave (CDW) insulator with a bonddisproportionated structure, similar to what is observed in BKBO30

  • We find evidence for a metallic phase where holes are strongly correlated with local structural distortions, forming a polaron-liquid-like phase

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Summary

Introduction

Lattice dimerization, referring to an alternation of two lattice constants, occurs in many quantum materials, including the organic charge-transfer solids[1,2,3], and perovskites systems like the rare-earth nickelates RNiO34–6, and the high-temperature (high-Tc) superconducting bismuthates Bi1−xKxBiO3 (BKBO)[7,8]. It is necessary to study this model in higher dimensions in the context of materials like RNiO3 and BKBO. We focus on BKBO and study how the SSH-type e–ph interaction produces both insulating and superconducting states as a function of doping. BKBO is in the so-called “negative charge transfer” regime[23,24,25,26], where holes self-dope from the cation to the ligand oxygen atoms. The subsequent hybridization between the cation and the oxygen atoms leads to a sizable e–ph interaction[6,7], which may be further enhanced by correlations[27], and is believed to drive a high-temperature metal-to-insulator (MIT) transition. The insulating state has a dimerized (or “bond disproportionated”) structure with expanded and collapsed

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