<HashMap><database>biostudies-literature</database><scores/><additional><omics_type>Unknown</omics_type><volume>17(1)</volume><submitter>Chen Y</submitter><pubmed_abstract>A recent experiment has reported unconventional superconductivity in twisted bilayer MoTe&lt;sub>2&lt;/sub>, emerging from a normal state that exhibits a finite anomalous Hall effect - a signature of intrinsic chirality. Motivated by this discovery, we construct a continuum model for twisted MoTe&lt;sub>2&lt;/sub> constrained by lattice symmetries from first-principles calculations that captures the moiré-induced inversion symmetry breaking even in the absence of a displacement field. Building on this model, we show that overscreening of the nominally repulsive Coulomb interaction gives rise to finite-momentum superconductivity in this chiral moiré system. Remarkably, the finite-momentum superconducting state can arise solely from internal symmetry breaking of the moiré superlattice, differentiating it from previously studied cases that require external fields. It further features a nonreciprocal quasiparticle dispersion and an intrinsic superconducting diode effect. Our results highlight a novel route to unconventional superconducting states in twisted transition metal dichalcogenides moiré systems, driven entirely by intrinsic symmetry-breaking effects.</pubmed_abstract><journal>Nature communications</journal><pagination>1077</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC12852829</full_dataset_link><repository>biostudies-literature</repository><pubmed_title>Finite-momentum superconductivity from chiral bands in twisted MoTe&lt;sub>2&lt;/sub>.</pubmed_title><pmcid>PMC12852829</pmcid><pubmed_authors>Schrade C</pubmed_authors><pubmed_authors>Zhang Y</pubmed_authors><pubmed_authors>Xu C</pubmed_authors><pubmed_authors>Chen Y</pubmed_authors></additional><is_claimable>false</is_claimable><name>Finite-momentum superconductivity from chiral bands in twisted MoTe&lt;sub>2&lt;/sub>.</name><description>A recent experiment has reported unconventional superconductivity in twisted bilayer MoTe&lt;sub>2&lt;/sub>, emerging from a normal state that exhibits a finite anomalous Hall effect - a signature of intrinsic chirality. Motivated by this discovery, we construct a continuum model for twisted MoTe&lt;sub>2&lt;/sub> constrained by lattice symmetries from first-principles calculations that captures the moiré-induced inversion symmetry breaking even in the absence of a displacement field. Building on this model, we show that overscreening of the nominally repulsive Coulomb interaction gives rise to finite-momentum superconductivity in this chiral moiré system. Remarkably, the finite-momentum superconducting state can arise solely from internal symmetry breaking of the moiré superlattice, differentiating it from previously studied cases that require external fields. It further features a nonreciprocal quasiparticle dispersion and an intrinsic superconducting diode effect. Our results highlight a novel route to unconventional superconducting states in twisted transition metal dichalcogenides moiré systems, driven entirely by intrinsic symmetry-breaking effects.</description><dates><release>2026-01-01T00:00:00Z</release><publication>2026 Jan</publication><modification>2026-06-16T07:25:13.571Z</modification><creation>2026-06-16T03:09:57.381Z</creation></dates><accession>S-EPMC12852829</accession><cross_references><pubmed>41501028</pubmed><doi>10.1038/s41467-025-67836-9</doi></cross_references></HashMap>