Strong pairing from doping-induced Feshbach resonance and second Fermi liquid through doping a bilayer spin-one Mott insulator: application to La$_3$Ni$_2$O$_7$ : Part I

Recently, a 80 K superconductor was discovered in La$_3$Ni$_2$O$_7$ under high pressure. Density function theory (DFT) calculations identify $d_{x^2-y^2}$, $d_{z^2}$ as the active orbitals on the bilayer square lattice with a $d^{8-x}$ configuration of of Ni per site. One naive expectation is to describe this system in terms of a two-orbital t-J model. 

However, we emphasize the importance of the Hund's coupling $J_H$ and the $x=0$ limit should be viewed as a spin-one Mott insulator.

Especially, the significant Hund's coupling shares the inter-layer super-exchange $J_perp$ of the $d_{z^2}$ orbital to the $d_{x^2-y^2}$ orbital, an effect that cannot be captured by conventional perturbation or mean-field approaches.In this study, we first explore the limit where the $d_{z^2}$ orbital is Mott localized, dealing with an one-orbital bilayer t-J model focused on the $d_{x^2-y^2}$ orbital. Notably, we find that strong inter-layer pairing survives up to $x=0.5$ hole doping driven by the transmitted $J_perp$, which explains the existence of high Tc superconductor in the experiment at this doping level. Next, we uncover the more realistic situation where the $d_{z^2}$ orbital is slightly hole doped and cannot be simply integrated out. We take the $J_H ightarrow +infty$ limit and propose a type II t-J model with four extit{spin-half} singlon ($d^7$) states and three extit{spin-one} doublon ($d^8$) states. Employing a parton mean field approach, we recover the similar results as in the one-orbital t-J model, but now with the effect of the $J_perp$ automatically generated.

Our calculations demonstrate that the pairing strength decreases with the hole doping $x$ and $x=0.5$ is likely larger than the optimal doping. We propose future experiments to electron dope the system to enhance $T_c$ further. We further present the Feshbach resonance and the Bardeen-Cooper-Schrieffer (BCS) to the Bose-Einstein condensation (BEC) 

with the numerical calculations.