Anomalous superconductivity and its competition with antiferromagnetism in doped Mott insulators
S. S. Kancharla, B. Kyung, D. Senechal, M. Civelli, M. Capone, G., Kotliar, A.-M.S. Tremblay

TL;DR
This study uses Cellular Dynamical Mean Field Theory to analyze the competition between antiferromagnetism and d-wave superconductivity in doped Mott insulators, revealing phase diagram features consistent with cuprate experiments.
Contribution
It provides a quantitative phase diagram of the Hubbard model showing the doping dependence of superconductivity and antiferromagnetism, incorporating realistic band parameters and electron-hole asymmetry.
Findings
d-wave order parameter scales with superexchange J
dome-shaped doping dependence of the order parameter
phase diagram matches experimental electron-hole asymmetry
Abstract
Proximity to a Mott insulating phase is likely to be an important physical ingredient of a theory that aims to describe high-temperature superconductivity in the cuprates. Quantum cluster methods are well suited to describe the Mott phase. Hence, as a step towards a quantitative theory of the competition between antiferromagnetism (AFM) and d-wave superconductivity (SC) in the cuprates, we use Cellular Dynamical Mean Field Theory to compute zero temperature properties of the two-dimensional square lattice Hubbard model. The d-wave order parameter is found to scale like the superexchange coupling J for on-site interaction U comparable to or larger than the bandwidth. The order parameter also assumes a dome shape as a function of doping while, by contrast, the gap in the single-particle density of states decreases monotonically with increasing doping. In the presence of a finite…
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