Abstract

The Mott insulating phase of the parent compounds is frequently taken as starting point for the underdoped high-$T_c$ cuprate superconductors. In particular, the pseudogap state is often considered as deriving from the Mott insulator. In this work, we systematically investigate different weakly-doped Mott insulators on the square and triangular lattice to clarify the relationship between the pseudogap and Mottness. We show that doping a two-dimensional Mott insulator does not necessarily lead to a pseudogap phase. Despite its inherent strong-coupling nature, we find that the existence or absence of a pseudogap depends sensitively on non-interacting band parameters and identify the crucial role played by the van Hove singularities of the system. Motivated by a SU(2) gauge theory for the pseudogap state, we propose and verify numerically a simple equation that governs the evolution of characteristic features in the electronic scattering rate.

Highlights

  • The complex phenomenology of cuprate high-Tc superconductors is widely thought of as a consequence of introducing mobile charge carriers in a Mott insulator through doping [1]

  • To shed light on the role played by AF correlations and Mottness, we address in this work the following fundamental question: do all doped Mott insulators with short-range AF correlations have a PG in two dimensions? To this end, we systematically study Hubbard models on square and triangular lattices, which have very different magnetic frustration properties

  • We have systematically analyzed which conditions are favorable for the emergence of a PG when doping insulating half-filled Hubbard models

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Summary

INTRODUCTION

The complex phenomenology of cuprate high-Tc superconductors is widely thought of as a consequence of introducing mobile charge carriers in a Mott insulator through doping [1]. Regarding the origin of the PG state, different approaches point to shortrange antiferromagnetic (AF) correlations and proximity to Mottness, including quantum Monte Carlo [22,23,24], exact diagonalization [20], cluster perturbation theory [25], and cluster extensions of dynamical mean-field theory (DMFT) [26,27,28,29,30,31] This is in line with a recent systematic experimental study [32] indicating that all other instabilities are secondary to AF correlations in the opening of the PG. This equation agrees with an SU(2) gauge theory [10,11,12], where the PG is the result of a Higgs mechanism, physically corresponding to local AF order with large orientational fluctuations

MODEL AND METHOD
TRIANGULAR LATTICE
SQUARE LATTICE
QUASIPOLE OF SELF-ENERGY IN A PG REGIME
Findings
CONCLUSION AND DISCUSSION
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