Transition from $s_{\pm }$-wave to $d_{x^2-y^2}$-wave superconductivity driven by interlayer interaction in the bilayer two-orbital model of La${}_3$Ni${}_2$O${}_7$

Abstract

We utilize the fluctuation-exchange approximation on a bilayer two-orbital model, incorporating $d_{x^2-y^2}$ and $d_{z^2}$ orbitals, to explore potential pairing symmetries in the bilayer nickelate La${}_3$Ni${}_2$O${}_7$. Our study particularly examines the impact of interlayer Coulomb interactions. In the absence of these interactions, the superconducting gap exhibits $s_{\pm }$-wave symmetry, with predominant intraorbital pairing in the $d_{z^2}$ orbital. As interlayer interactions increase, $s_{\pm }$-wave superconductivity is suppressed, while the superconductivity with a $d_{x^2-y^2}$-wave gap is enhanced, resulting in a transition at a critical interaction strength. This $d_{x^2-y^2}$-wave superconductivity is distinct not only from the $s_{\pm }$-wave superconductivity but also from the intraorbital $d$-wave pairing in cuprate superconductors, as it is dominated by the interlayer pairing between the $d_{x^2-y^2}$ and $d_{z^2}$ orbitals. Additionally, charge fluctuations play a crucial role in driving the transition from $s_{\pm }$ wave to $d_{x^2-y^2}$ wave superconductivity. Our findings indicate that interlayer Coulomb interactions are crucial for understanding the pairing mechanism in La${}_3$Ni${}_2$O${}_7$.

11 pages, 8 figures

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