{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:3RFKXECE5JNQSSVPZJFBOKVBQ2","short_pith_number":"pith:3RFKXECE","schema_version":"1.0","canonical_sha256":"dc4aab9044ea5b094aafca4a172aa186bd319997ca96f3b87000c85760efc4a2","source":{"kind":"arxiv","id":"2601.05933","version":2},"attestation_state":"computed","paper":{"title":"Phase-space networks and connectivity of the kagome antiferromagnet","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.stat-mech","authors_text":"Brandon B. Le, Gia-Wei Chern, Seung-Hun Lee","submitted_at":"2026-01-09T16:47:01Z","abstract_excerpt":"We study the coplanar ground-state manifold of the kagome Heisenberg antiferromagnet using a phase-space network representation, in which nodes correspond to coplanar ground states and edges represent transitions generated by weathervane loop rotations. In the coplanar manifold, each configuration can be mapped to a three-coloring problem on the dual honeycomb lattice, where a weathervane mode corresponds to a closed loop of two alternating colors. By comparing networks that include all weathervane loops with networks restricted to elementary six-spin loops, we examine how energetic constraint"},"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":"2601.05933","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-01-09T16:47:01Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"f17b61aaf5b037a3b0340eb040cd24d53fbf8d9929b057d4110510184d665033","abstract_canon_sha256":"ee93b099e673015bfeea8aafcd1afa3cde79e2c58fd0514820694df63028917b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-05T00:41:16.363558Z","signature_b64":"zOu/6WZ4ut3sG7CQHNfvzqTVoHm8/eQ5Eo10d77PnabWpBjIAPynXaNeSjHOkT4so1F+mjp1EMtGmnaNlw4eAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dc4aab9044ea5b094aafca4a172aa186bd319997ca96f3b87000c85760efc4a2","last_reissued_at":"2026-08-05T00:41:16.360887Z","signature_status":"signed_v1","first_computed_at":"2026-08-05T00:41:16.360887Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase-space networks and connectivity of the kagome antiferromagnet","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.stat-mech","authors_text":"Brandon B. Le, Gia-Wei Chern, Seung-Hun Lee","submitted_at":"2026-01-09T16:47:01Z","abstract_excerpt":"We study the coplanar ground-state manifold of the kagome Heisenberg antiferromagnet using a phase-space network representation, in which nodes correspond to coplanar ground states and edges represent transitions generated by weathervane loop rotations. In the coplanar manifold, each configuration can be mapped to a three-coloring problem on the dual honeycomb lattice, where a weathervane mode corresponds to a closed loop of two alternating colors. By comparing networks that include all weathervane loops with networks restricted to elementary six-spin loops, we examine how energetic constraint"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2601.05933","kind":"arxiv","version":2},"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/2601.05933/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":"2601.05933","created_at":"2026-08-05T00:41:16.361735+00:00"},{"alias_kind":"arxiv_version","alias_value":"2601.05933v2","created_at":"2026-08-05T00:41:16.361735+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2601.05933","created_at":"2026-08-05T00:41:16.361735+00:00"},{"alias_kind":"pith_short_12","alias_value":"3RFKXECE5JNQ","created_at":"2026-08-05T00:41:16.361735+00:00"},{"alias_kind":"pith_short_16","alias_value":"3RFKXECE5JNQSSVP","created_at":"2026-08-05T00:41:16.361735+00:00"},{"alias_kind":"pith_short_8","alias_value":"3RFKXECE","created_at":"2026-08-05T00:41:16.361735+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.02512","citing_title":"Frustrated neurons: Energy landscapes and relaxation dynamics in repulsive phase oscillators","ref_index":48,"is_internal_anchor":true},{"citing_arxiv_id":"2604.18902","citing_title":"Energy landscape of the kagome antiferromagnet: Characterization of multiple energy scales","ref_index":38,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3RFKXECE5JNQSSVPZJFBOKVBQ2","json":"https://pith.science/pith/3RFKXECE5JNQSSVPZJFBOKVBQ2.json","graph_json":"https://pith.science/api/pith-number/3RFKXECE5JNQSSVPZJFBOKVBQ2/graph.json","events_json":"https://pith.science/api/pith-number/3RFKXECE5JNQSSVPZJFBOKVBQ2/events.json","paper":"https://pith.science/paper/3RFKXECE"},"agent_actions":{"view_html":"https://pith.science/pith/3RFKXECE5JNQSSVPZJFBOKVBQ2","download_json":"https://pith.science/pith/3RFKXECE5JNQSSVPZJFBOKVBQ2.json","view_paper":"https://pith.science/paper/3RFKXECE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2601.05933&json=true","fetch_graph":"https://pith.science/api/pith-number/3RFKXECE5JNQSSVPZJFBOKVBQ2/graph.json","fetch_events":"https://pith.science/api/pith-number/3RFKXECE5JNQSSVPZJFBOKVBQ2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3RFKXECE5JNQSSVPZJFBOKVBQ2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3RFKXECE5JNQSSVPZJFBOKVBQ2/action/storage_attestation","attest_author":"https://pith.science/pith/3RFKXECE5JNQSSVPZJFBOKVBQ2/action/author_attestation","sign_citation":"https://pith.science/pith/3RFKXECE5JNQSSVPZJFBOKVBQ2/action/citation_signature","submit_replication":"https://pith.science/pith/3RFKXECE5JNQSSVPZJFBOKVBQ2/action/replication_record"}},"created_at":"2026-08-05T00:41:16.361735+00:00","updated_at":"2026-08-05T00:41:16.361735+00:00"}