{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:AOHSD5RDE45B33FOSWRDF5PK3Y","short_pith_number":"pith:AOHSD5RD","schema_version":"1.0","canonical_sha256":"038f21f623273a1decae95a232f5eade356e3a1004207964547f98a8297b5fda","source":{"kind":"arxiv","id":"2506.07741","version":1},"attestation_state":"computed","paper":{"title":"Interlayer Pairing in Bilayer Nickelates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Adriana Moreo, Elbio Dagotto, Ling-Fang Lin, Peter Doak, Thomas A. Maier, Yang Zhang","submitted_at":"2025-06-09T13:24:14Z","abstract_excerpt":"The discovery of $T_c\\sim 80$~K superconductivity in pressurized La$_3$Ni$_2$O$_7$ has launched a new platform to study high-temperature superconductivity. Using non-perturbative dynamic cluster approximation quantum Monte Carlo calculations, we characterize the magnetic and superconducting pairing behavior of a realistic bilayer two-orbital Hubbard-Hund model of this system that describes the relevant Ni $e_g$ states with physically relevant interaction strengths. We find a leading $s^\\pm$ superconducting instability in this model and show that this state primarily arises from interlayer pair"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2506.07741","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-06-09T13:24:14Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"4dca474fd8cc9a91d5ebb63c48b5d43d104ff0a3c50c7a6843e90ce1138dce4a","abstract_canon_sha256":"bc3c60fd60977a32527c50609b2f8087f496a12be26cfbb8c7ddce80d89effb7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:18:32.533616Z","signature_b64":"ygmgpXBwFLKTFLoN0q6sKUHl7JEzhbSKt/1aoWA4aq1i46srpQ27K5zCL0UiaZGEhPFdY9UgFxR/LF7B7+XECg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"038f21f623273a1decae95a232f5eade356e3a1004207964547f98a8297b5fda","last_reissued_at":"2026-07-05T11:18:32.533100Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:18:32.533100Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Interlayer Pairing in Bilayer Nickelates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Adriana Moreo, Elbio Dagotto, Ling-Fang Lin, Peter Doak, Thomas A. Maier, Yang Zhang","submitted_at":"2025-06-09T13:24:14Z","abstract_excerpt":"The discovery of $T_c\\sim 80$~K superconductivity in pressurized La$_3$Ni$_2$O$_7$ has launched a new platform to study high-temperature superconductivity. Using non-perturbative dynamic cluster approximation quantum Monte Carlo calculations, we characterize the magnetic and superconducting pairing behavior of a realistic bilayer two-orbital Hubbard-Hund model of this system that describes the relevant Ni $e_g$ states with physically relevant interaction strengths. We find a leading $s^\\pm$ superconducting instability in this model and show that this state primarily arises from interlayer pair"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.07741","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2506.07741/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2506.07741","created_at":"2026-07-05T11:18:32.533149+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.07741v1","created_at":"2026-07-05T11:18:32.533149+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.07741","created_at":"2026-07-05T11:18:32.533149+00:00"},{"alias_kind":"pith_short_12","alias_value":"AOHSD5RDE45B","created_at":"2026-07-05T11:18:32.533149+00:00"},{"alias_kind":"pith_short_16","alias_value":"AOHSD5RDE45B33FO","created_at":"2026-07-05T11:18:32.533149+00:00"},{"alias_kind":"pith_short_8","alias_value":"AOHSD5RD","created_at":"2026-07-05T11:18:32.533149+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.30297","citing_title":"Electron Doping of $\\mathrm{La_3Ni_2O_7}$ Thin Films: Candidate Metal Dopants and Their Potential Impact on Superconductivity","ref_index":49,"is_internal_anchor":false},{"citing_arxiv_id":"2505.07394","citing_title":"Correlated electronic structure of the alternating monolayer-bilayer nickelate La$_{5}$Ni$_{3}$O$_{11}$","ref_index":49,"is_internal_anchor":false},{"citing_arxiv_id":"2506.20497","citing_title":"Theoretical study on ambient pressure superconductivity in La$_3$Ni$_2$O$_7$ thin films : structural analysis, model construction, and robustness of $s\\pm$-wave pairing","ref_index":67,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AOHSD5RDE45B33FOSWRDF5PK3Y","json":"https://pith.science/pith/AOHSD5RDE45B33FOSWRDF5PK3Y.json","graph_json":"https://pith.science/api/pith-number/AOHSD5RDE45B33FOSWRDF5PK3Y/graph.json","events_json":"https://pith.science/api/pith-number/AOHSD5RDE45B33FOSWRDF5PK3Y/events.json","paper":"https://pith.science/paper/AOHSD5RD"},"agent_actions":{"view_html":"https://pith.science/pith/AOHSD5RDE45B33FOSWRDF5PK3Y","download_json":"https://pith.science/pith/AOHSD5RDE45B33FOSWRDF5PK3Y.json","view_paper":"https://pith.science/paper/AOHSD5RD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.07741&json=true","fetch_graph":"https://pith.science/api/pith-number/AOHSD5RDE45B33FOSWRDF5PK3Y/graph.json","fetch_events":"https://pith.science/api/pith-number/AOHSD5RDE45B33FOSWRDF5PK3Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AOHSD5RDE45B33FOSWRDF5PK3Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AOHSD5RDE45B33FOSWRDF5PK3Y/action/storage_attestation","attest_author":"https://pith.science/pith/AOHSD5RDE45B33FOSWRDF5PK3Y/action/author_attestation","sign_citation":"https://pith.science/pith/AOHSD5RDE45B33FOSWRDF5PK3Y/action/citation_signature","submit_replication":"https://pith.science/pith/AOHSD5RDE45B33FOSWRDF5PK3Y/action/replication_record"}},"created_at":"2026-07-05T11:18:32.533149+00:00","updated_at":"2026-07-05T11:18:32.533149+00:00"}