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Compressive Strain Turns s±s^{\pm} into dd-Wave Pairing in One-unit-cell La3_3Ni2_2O7_7 Thin Film Via Substrate-Induced Hole Doping

Published 22 Dec 2025 in cond-mat.supr-con and cond-mat.str-el | (2512.19520v1)

Abstract: Motivated by recent reports of ambient-pressure superconductivity in La<em>3<em>3Ni2_2O7_7 films grown on LaSrAlO4_4, we investigate the superconducting instability in a one-unit cell thin film using {\it ab initio} and random-phase approximation techniques. Compared to the high-pressure bulk system, the ratio of inter-layer d</em>3z<sup>2r<sup>2d</em>{3z<sup>2-r<sup>2} hopping to intra-layer dx<sup>2y<sup>2d_{x<sup>2-y<sup>2} hopping is suppressed in the 1UC thin film, and the crystal-field splitting of the ege_g orbitals is increased. Our calculation indicates that spin-fluctuation-driven pairing correlations are weak for the stoichiometric case at ambient pressure, but increase significantly under hole doping. The leading pairing symmetry is also found to change by hole doping. Specifically, we obtain a leading dx<sup>2y<sup>2d_{x<sup>2-y<sup>2} pairing state at moderate hole doping, followed by a dxyd_{xy} state at higher doping. These states are driven by intra-band spin-fluctuation scattering {\it within} the γγ hole pocket centered around the M point, and arise primarily from states in the Ni layer {\it farther} from the substrate. These results strongly suggest that the thin-film superconducting samples are hole-doped and that pairing in this system predominantly arises in the layer, as opposed to the inter-layer pairing in the pressurized bulk system.

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