The recent experimental observations of high-temperature superconductivity in bilayer nickelate have attracted much attention. Previous studies have assumed a mirror symmetry $\mathcal{M}$ between the two layers and focused on uniform and clean superconducting states. Here, we show that breaking this mirror symmetry via an applied displacement field can stabilize a pair-density-wave (PDW) superconductor, which is similar to the Fulde-Ferrell-Larkin-Ovchinnikov state, but at zero magnetic field. Based on a mean-field analysis of a model of a $d_{x^2-y^2}$ orbital with an effective interlayer attraction, we demonstrate that the PDW phase is robust over a wide range of displacement field, interlayer hopping strengths, and electron fillings. Finally, we analyze disorder effects on interlayer superconductivity within the first Born approximation. Based on symmetry considerations, we show that pairing is weakened by disorders which break the mirror symmetry, even with unbroken time-reversal symmetry. Our results establish bilayer nickelate as a tunable platform for realizing finite-momentum pairing and for exploring generalized disorder effects.

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• Pair density wave
• Superconductivity
• Nickelates