In order to explore the reason why the single-layered cuprates, La$_{ 2-x}$(Sr/Ba)$_x$CuO$_4$ ($T_c\simeq$ 40K) and HgBa$_2$CuO$_{ 4+\delta}$ ($T_c\simeq$ 90K), have such a significant difference in $T_c$, we study a two-orbital model that incorporates the $d_{ z^2}$ orbital on top of the $d_{ x^2-y^2}$ orbital. It is found, with the fluctuation exchange approximation, that the $d_{ z^2}$ orbital contribution to the Fermi surface, which is stronger in the La system, works against d-wave superconductivity, thereby dominating over the effect of the Fermi surface shape. The result resolves the long-standing contradiction between the theoretical results on Hubbard-type models and the experimental material dependence of $T_c$ in the cuprates.
Categories: cond-mat.supr-con