{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:XOIMUJCB2QTNSLWSGZDYQWA5SH","short_pith_number":"pith:XOIMUJCB","schema_version":"1.0","canonical_sha256":"bb90ca2441d426d92ed2364788581d91f85fa8bc297555401c7b03bf3e0b8ec6","source":{"kind":"arxiv","id":"2503.21769","version":1},"attestation_state":"computed","paper":{"title":"Kondo-lattice phenomenology of twisted bilayer WSe$_2$ from compact molecular orbitals of topological bands","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Chenyuan Li, Fang Xie, Jennifer Cano, Qimiao Si","submitted_at":"2025-03-27T17:59:08Z","abstract_excerpt":"The discovery of superconductivity and correlated electronic phases in twisted bilayer WSe$_2$ (Xia et al., Nature 2024; Guo et al., Nature 2025) has generated considerable excitement. Accompanying the superconductivity and a correlated insulator phase is the Kondo-lattice-like phenomenology in transport properties. Here we consider how such phenomenology can develop when the combination of the active bands are topological. We advance a unique construction of compact molecular orbitals through a partial Wannierization that is symmetry preserving. The resulting Anderson lattice model provides t"},"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":"2503.21769","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-03-27T17:59:08Z","cross_cats_sorted":[],"title_canon_sha256":"86fff0e724408b8c0bd3f214653a649945b013a912021b18dd1d3dfb0322396a","abstract_canon_sha256":"724917bcbcf1a627704b69b48bcc274af7d5e5c485a2ea98ba13db41fc369563"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:40:30.399839Z","signature_b64":"ZlSprr8pxcObRwTfWYdBq/bfkQoZODnBsPTR+asxl7jOFpn0d8jWsa4KymiBup2mt5LkjijAGRCM1SHxmZAxCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb90ca2441d426d92ed2364788581d91f85fa8bc297555401c7b03bf3e0b8ec6","last_reissued_at":"2026-07-05T10:40:30.399352Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:40:30.399352Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Kondo-lattice phenomenology of twisted bilayer WSe$_2$ from compact molecular orbitals of topological bands","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Chenyuan Li, Fang Xie, Jennifer Cano, Qimiao Si","submitted_at":"2025-03-27T17:59:08Z","abstract_excerpt":"The discovery of superconductivity and correlated electronic phases in twisted bilayer WSe$_2$ (Xia et al., Nature 2024; Guo et al., Nature 2025) has generated considerable excitement. Accompanying the superconductivity and a correlated insulator phase is the Kondo-lattice-like phenomenology in transport properties. Here we consider how such phenomenology can develop when the combination of the active bands are topological. We advance a unique construction of compact molecular orbitals through a partial Wannierization that is symmetry preserving. The resulting Anderson lattice model provides t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.21769","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/2503.21769/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":"2503.21769","created_at":"2026-07-05T10:40:30.399416+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.21769v1","created_at":"2026-07-05T10:40:30.399416+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.21769","created_at":"2026-07-05T10:40:30.399416+00:00"},{"alias_kind":"pith_short_12","alias_value":"XOIMUJCB2QTN","created_at":"2026-07-05T10:40:30.399416+00:00"},{"alias_kind":"pith_short_16","alias_value":"XOIMUJCB2QTNSLWS","created_at":"2026-07-05T10:40:30.399416+00:00"},{"alias_kind":"pith_short_8","alias_value":"XOIMUJCB","created_at":"2026-07-05T10:40:30.399416+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.03766","citing_title":"Gossamer Superconductivity in Moir\\'e WSe$_2$ Bilayer","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03766","citing_title":"Gossamer Superconductivity in Moir\\'e WSe$_2$ Bilayer","ref_index":38,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XOIMUJCB2QTNSLWSGZDYQWA5SH","json":"https://pith.science/pith/XOIMUJCB2QTNSLWSGZDYQWA5SH.json","graph_json":"https://pith.science/api/pith-number/XOIMUJCB2QTNSLWSGZDYQWA5SH/graph.json","events_json":"https://pith.science/api/pith-number/XOIMUJCB2QTNSLWSGZDYQWA5SH/events.json","paper":"https://pith.science/paper/XOIMUJCB"},"agent_actions":{"view_html":"https://pith.science/pith/XOIMUJCB2QTNSLWSGZDYQWA5SH","download_json":"https://pith.science/pith/XOIMUJCB2QTNSLWSGZDYQWA5SH.json","view_paper":"https://pith.science/paper/XOIMUJCB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.21769&json=true","fetch_graph":"https://pith.science/api/pith-number/XOIMUJCB2QTNSLWSGZDYQWA5SH/graph.json","fetch_events":"https://pith.science/api/pith-number/XOIMUJCB2QTNSLWSGZDYQWA5SH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XOIMUJCB2QTNSLWSGZDYQWA5SH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XOIMUJCB2QTNSLWSGZDYQWA5SH/action/storage_attestation","attest_author":"https://pith.science/pith/XOIMUJCB2QTNSLWSGZDYQWA5SH/action/author_attestation","sign_citation":"https://pith.science/pith/XOIMUJCB2QTNSLWSGZDYQWA5SH/action/citation_signature","submit_replication":"https://pith.science/pith/XOIMUJCB2QTNSLWSGZDYQWA5SH/action/replication_record"}},"created_at":"2026-07-05T10:40:30.399416+00:00","updated_at":"2026-07-05T10:40:30.399416+00:00"}