Superconductivity in 1313 La3Ni2O7 resides in the hole-doped trilayer subsystem with s±-wave pairing, weakened by doping and S-N-S Josephson coupling from the Mott-insulating single-layer subsystem.
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La5Ni3O11 shows layer-selective physics with the single layer near a Mott instability and the bilayer dominating low-energy states, yielding an electronic structure that closely resembles the bilayer La3Ni2O7.
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Pairing mechanism and superconductivity in 1313 phase La$_3$Ni$_2$O$_7$
Superconductivity in 1313 La3Ni2O7 resides in the hole-doped trilayer subsystem with s±-wave pairing, weakened by doping and S-N-S Josephson coupling from the Mott-insulating single-layer subsystem.
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Correlated electronic structure of the alternating monolayer-bilayer nickelate La$_{5}$Ni$_{3}$O$_{11}$
La5Ni3O11 shows layer-selective physics with the single layer near a Mott instability and the bilayer dominating low-energy states, yielding an electronic structure that closely resembles the bilayer La3Ni2O7.