{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:UB55M5IKFG7OMKJUTHFRCGCOXT","short_pith_number":"pith:UB55M5IK","schema_version":"1.0","canonical_sha256":"a07bd6750a29bee6293499cb11184ebcf5f2e69c123dc31cbc5fee6363866cc1","source":{"kind":"arxiv","id":"2403.11063","version":1},"attestation_state":"computed","paper":{"title":"Emergent Haldane Model and Photon-Valley Locking in Chiral Cavities","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.other"],"primary_cat":"cond-mat.mes-hall","authors_text":"Liu Yang, Qing-Dong Jiang","submitted_at":"2024-03-17T02:33:11Z","abstract_excerpt":"The realization of Haldane's topological graphene model in practical materials has presented significant challenges. Here, we propose achieving this model by embedding graphene in chiral cavities, using the asymptotically decoupled framework detailed in Ref. [Phys. Rev. Lett. 126, 153603 (2021)]. Additionally, we introduce an equilibrium strategy for achieving valley polarization in this system with C2-symmetry breaking. Through numerical methods, we quantify the locking of photon numbers with Bloch electrons and calculate the topology-induced imbalance of valley photons. Furthermore, we eluci"},"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":"2403.11063","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-03-17T02:33:11Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.other"],"title_canon_sha256":"7a7e3a6bb7377ab3c3d69a16dc80eeb353b8f65c99cd02176e73261595edd110","abstract_canon_sha256":"ac79114182bf629303ceb6677246639c858d3104dcd646758e9b3acb4c6570fd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:42:34.660477Z","signature_b64":"xmZTul9nia8Z3lDDz289qO7WJ5TBSE5o47T44tOzxz7hJDVwT5Tf8H+egAeCTVwOaEpkAL5bbDNyfIDw/WJrDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a07bd6750a29bee6293499cb11184ebcf5f2e69c123dc31cbc5fee6363866cc1","last_reissued_at":"2026-07-05T10:42:34.659866Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:42:34.659866Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergent Haldane Model and Photon-Valley Locking in Chiral Cavities","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.other"],"primary_cat":"cond-mat.mes-hall","authors_text":"Liu Yang, Qing-Dong Jiang","submitted_at":"2024-03-17T02:33:11Z","abstract_excerpt":"The realization of Haldane's topological graphene model in practical materials has presented significant challenges. Here, we propose achieving this model by embedding graphene in chiral cavities, using the asymptotically decoupled framework detailed in Ref. [Phys. Rev. Lett. 126, 153603 (2021)]. Additionally, we introduce an equilibrium strategy for achieving valley polarization in this system with C2-symmetry breaking. Through numerical methods, we quantify the locking of photon numbers with Bloch electrons and calculate the topology-induced imbalance of valley photons. Furthermore, we eluci"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.11063","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/2403.11063/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":"2403.11063","created_at":"2026-07-05T10:42:34.659934+00:00"},{"alias_kind":"arxiv_version","alias_value":"2403.11063v1","created_at":"2026-07-05T10:42:34.659934+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.11063","created_at":"2026-07-05T10:42:34.659934+00:00"},{"alias_kind":"pith_short_12","alias_value":"UB55M5IKFG7O","created_at":"2026-07-05T10:42:34.659934+00:00"},{"alias_kind":"pith_short_16","alias_value":"UB55M5IKFG7OMKJU","created_at":"2026-07-05T10:42:34.659934+00:00"},{"alias_kind":"pith_short_8","alias_value":"UB55M5IK","created_at":"2026-07-05T10:42:34.659934+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.12163","citing_title":"Non-Hermitian wave-packet dynamics and its realization within a non-Hermitian chiral cavity","ref_index":43,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UB55M5IKFG7OMKJUTHFRCGCOXT","json":"https://pith.science/pith/UB55M5IKFG7OMKJUTHFRCGCOXT.json","graph_json":"https://pith.science/api/pith-number/UB55M5IKFG7OMKJUTHFRCGCOXT/graph.json","events_json":"https://pith.science/api/pith-number/UB55M5IKFG7OMKJUTHFRCGCOXT/events.json","paper":"https://pith.science/paper/UB55M5IK"},"agent_actions":{"view_html":"https://pith.science/pith/UB55M5IKFG7OMKJUTHFRCGCOXT","download_json":"https://pith.science/pith/UB55M5IKFG7OMKJUTHFRCGCOXT.json","view_paper":"https://pith.science/paper/UB55M5IK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2403.11063&json=true","fetch_graph":"https://pith.science/api/pith-number/UB55M5IKFG7OMKJUTHFRCGCOXT/graph.json","fetch_events":"https://pith.science/api/pith-number/UB55M5IKFG7OMKJUTHFRCGCOXT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UB55M5IKFG7OMKJUTHFRCGCOXT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UB55M5IKFG7OMKJUTHFRCGCOXT/action/storage_attestation","attest_author":"https://pith.science/pith/UB55M5IKFG7OMKJUTHFRCGCOXT/action/author_attestation","sign_citation":"https://pith.science/pith/UB55M5IKFG7OMKJUTHFRCGCOXT/action/citation_signature","submit_replication":"https://pith.science/pith/UB55M5IKFG7OMKJUTHFRCGCOXT/action/replication_record"}},"created_at":"2026-07-05T10:42:34.659934+00:00","updated_at":"2026-07-05T10:42:34.659934+00:00"}