Extremely Correlated Fermi Liquid theory for $U=\infty$, $d=\infty$ Hubbard model to ${\cal O}(\lambda^3)$

TL;DR

This paper advances the extremely correlated Fermi liquid theory by calculating third-order $\

Contribution

It provides third-order $\

Findings

All methods show quadratic T resistivity transitioning to linear T in strange metals.

The third-order calculations improve the accuracy of resistivity, self-energy, and quasiparticle weight estimates.

Comparison with DMFT validates the $\

Abstract

We present the ${\cal O}(\lambda^3)$ results from the $\lambda$ expansion in the extremely correlated Fermi liquid theory applied to the infinite-dimensional $t$-$J$ model (with $J=0$), and compare the results with the earlier ${\cal O}(\lambda^2)$ results as well as the results from the dynamical mean field theory. We focus attention on the $T$ dependence of the resistivity $\rho(T)$, the Dyson self energy, and the quasiparticle weight $Z$ at various densities. The comparison shows that all the methods display quadratic in T resistivity followed by a quasi-linear in T resistivity characterizing a strange metal, and gives an estimate of the different scales of these variables relative to the exact results.