{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:OJEDVWQTXEFFPFJKXGR3Q5NEON","short_pith_number":"pith:OJEDVWQT","schema_version":"1.0","canonical_sha256":"72483ada13b90a57952ab9a3b875a47354e3da5252adc3f8d7c26d7c4d9b109b","source":{"kind":"arxiv","id":"1107.1102","version":2},"attestation_state":"computed","paper":{"title":"Edge magnetism of Heisenberg model on honeycomb lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Hsiu-Hau Lin, Toshiya Hikihara, Wen-Min Huang, Yen-Chen Lee","submitted_at":"2011-07-06T11:48:06Z","abstract_excerpt":"In our previous study, a single-branch of ferromagnetic magnon with linear dispersion is shown to exist near the (uncompensated) zigzag edge for Heisenberg model on honeycomb lattice. Here we develop a field-theory description for the edge magnon and find its dynamics is captured by the one-dimensional relativistic Klein-Gordon equation. It is intriguing that the boundary field theory for the edge magnon is tied up with its bulk counterpart, described by the two-dimensional Klein-Gordon equation. Furthermore, we also reveal how the parity symmetry relates evanescent modes on opposite edges in "},"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":"1107.1102","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-07-06T11:48:06Z","cross_cats_sorted":[],"title_canon_sha256":"6dc274ddb119b2733f78c9176499f55fe1137adacf8fefc7f06b7e718ec83d8b","abstract_canon_sha256":"18e6470070fabed58fcf192f0cadf127f4fa0ec9b4b6af711c6d024594f225ec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:18:35.552550Z","signature_b64":"LW2ls6H7Pb0G4MlvJ1i1vKErSSL37ZT65c3MHTnawlc6aHogdATNexFb2uZ60pbmgsSjvbGduLvYhIxJW/VOCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"72483ada13b90a57952ab9a3b875a47354e3da5252adc3f8d7c26d7c4d9b109b","last_reissued_at":"2026-05-18T04:18:35.551971Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:18:35.551971Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Edge magnetism of Heisenberg model on honeycomb lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Hsiu-Hau Lin, Toshiya Hikihara, Wen-Min Huang, Yen-Chen Lee","submitted_at":"2011-07-06T11:48:06Z","abstract_excerpt":"In our previous study, a single-branch of ferromagnetic magnon with linear dispersion is shown to exist near the (uncompensated) zigzag edge for Heisenberg model on honeycomb lattice. Here we develop a field-theory description for the edge magnon and find its dynamics is captured by the one-dimensional relativistic Klein-Gordon equation. It is intriguing that the boundary field theory for the edge magnon is tied up with its bulk counterpart, described by the two-dimensional Klein-Gordon equation. Furthermore, we also reveal how the parity symmetry relates evanescent modes on opposite edges in "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.1102","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":""},"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":"1107.1102","created_at":"2026-05-18T04:18:35.552037+00:00"},{"alias_kind":"arxiv_version","alias_value":"1107.1102v2","created_at":"2026-05-18T04:18:35.552037+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.1102","created_at":"2026-05-18T04:18:35.552037+00:00"},{"alias_kind":"pith_short_12","alias_value":"OJEDVWQTXEFF","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_16","alias_value":"OJEDVWQTXEFFPFJK","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_8","alias_value":"OJEDVWQT","created_at":"2026-05-18T12:26:37.096874+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OJEDVWQTXEFFPFJKXGR3Q5NEON","json":"https://pith.science/pith/OJEDVWQTXEFFPFJKXGR3Q5NEON.json","graph_json":"https://pith.science/api/pith-number/OJEDVWQTXEFFPFJKXGR3Q5NEON/graph.json","events_json":"https://pith.science/api/pith-number/OJEDVWQTXEFFPFJKXGR3Q5NEON/events.json","paper":"https://pith.science/paper/OJEDVWQT"},"agent_actions":{"view_html":"https://pith.science/pith/OJEDVWQTXEFFPFJKXGR3Q5NEON","download_json":"https://pith.science/pith/OJEDVWQTXEFFPFJKXGR3Q5NEON.json","view_paper":"https://pith.science/paper/OJEDVWQT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1107.1102&json=true","fetch_graph":"https://pith.science/api/pith-number/OJEDVWQTXEFFPFJKXGR3Q5NEON/graph.json","fetch_events":"https://pith.science/api/pith-number/OJEDVWQTXEFFPFJKXGR3Q5NEON/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OJEDVWQTXEFFPFJKXGR3Q5NEON/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OJEDVWQTXEFFPFJKXGR3Q5NEON/action/storage_attestation","attest_author":"https://pith.science/pith/OJEDVWQTXEFFPFJKXGR3Q5NEON/action/author_attestation","sign_citation":"https://pith.science/pith/OJEDVWQTXEFFPFJKXGR3Q5NEON/action/citation_signature","submit_replication":"https://pith.science/pith/OJEDVWQTXEFFPFJKXGR3Q5NEON/action/replication_record"}},"created_at":"2026-05-18T04:18:35.552037+00:00","updated_at":"2026-05-18T04:18:35.552037+00:00"}