Abstract

We determine the ground-state phase diagram of the three-band Hubbard model across a range of model parameters using density matrix embedding theory. We study the atomic-scale nature of the antiferromagnetic (AFM) and superconducting (SC) orders, explicitly including the oxygen degrees of freedom. All parametrizations of the model display AFM and SC phases, but the decay of AFM order with doping is too slow compared to the experimental phase diagram, and further, coexistence of AFM and SC orders occurs in all parameter sets. The local magnetic moment localizes entirely at the copper sites. The magnetic phase diagram is particularly sensitive to $\Delta_{pd}$ and $t_{pp}$, and existing estimates of the charge transfer gap $\Delta_{pd}$ appear too large in so-called minimal model parametrizations. The electron-doped side of the phase diagram is qualitatively distinct from hole-doped side and we find an unusual two-peak structure in the SC in the full model parametrization. Examining the SC order at the atomic scale, within the larger scale $d_{x^2 - y^2}$-wave SC pairing order between Cu-Cu and O-O, we also observe a local $p_{x (y)}$ [or $d_{xz (yz)}$]-symmetry modulation of the pair density on the Cu-O bonds. Our work highlights some of the features that arise in a three-band versus one-band picture, the role of the oxygen degrees of freedom in new kinds of atomic-scale SC orders, and the necessity of re-evaluating current parametrizations of the three-band Hubbard model.

Highlights

  • The three-band Hubbard model, known as the Emery model [1], is generally believed to contain the essential physics of the high-Tc cuprates that arises from the interplay between the copper dx2−y2 and oxygen px(y) orbitals in the CuO2 layers

  • We studied the doping dependence of the ground-state of the model paying particular attention to the local antiferromagnetic (AFM) and superconducting (SC) orders

  • In a broad range of model parameters we find a decrease in AFM order upon doping and a SC dome

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Summary

INTRODUCTION

The three-band Hubbard model, known as the Emery model [1], is generally believed to contain the essential physics of the high-Tc cuprates that arises from the interplay between the copper dx2−y2 and oxygen px(y) orbitals in the CuO2 layers. We can use DMET to provide a detailed description of the ground-state phases and orders as a function of doping, including the doping asymmetry and atomic-scale orders that are new to the three-band case. Another complication of the three-band model is the much larger parameter space than the one-band case. Our findings provide insights into the detailed picture of magnetic and superconducting orders that is provided by three-band models

Model parametrization
Framework
Impurity and lattice
Impurity Hamiltonian and solver
DMET self-consistency
Order parameters
Charge and magnetic moments
Band gap
Orbital resolved band structure
Hole-doped phases with standard parametrizations
Range of reasonable parameters
Electron doped phases in the full model
Atomic scale orders in the full model
CONCLUSIONS
Full Text
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