{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:GME6UKKKQRWU2U5WSVHMF435LW","short_pith_number":"pith:GME6UKKK","schema_version":"1.0","canonical_sha256":"3309ea294a846d4d53b6954ec2f37d5d832dea070d0ea2a5412a41ba865ab904","source":{"kind":"arxiv","id":"1801.00962","version":1},"attestation_state":"computed","paper":{"title":"Investigation of the spin-1 honeycomb antiferromagnet BaNi$_2$V$_2$O$_8$ with easy plane anisotropy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Schneidewind, A. T. M. N. Islam, B. Klemke, B. Lake, E. A. Goremychkin, E. S. Klyushina, J. T. Park, M. M{\\aa}nsson, T. Guidi","submitted_at":"2018-01-03T11:31:58Z","abstract_excerpt":"The magnetic properties of the two-dimensional, S=1 honeycomb antiferromagnet BaNi$_2$V$_2$O$_8$ have been comprehensively studied using DC susceptibility measurements and inelastic neutron scattering techniques. The magnetic excitation spectrum is found to be dispersionless within experimental resolution between the honeycomb layers, while it disperses strongly within the honeycomb plane where it consists of two gapped spin-wave modes. The magnetic excitations are compared to linear spin-wave theory allowing the Hamiltonian to be determined. The first- and second-neighbour magnetic exchange i"},"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":"1801.00962","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-01-03T11:31:58Z","cross_cats_sorted":[],"title_canon_sha256":"32075171c5bc466b1e34cbf349fd5d570a202d429ae7dc117c09b0206a521b3f","abstract_canon_sha256":"ddf70bc25df5c0782b9ed79f41d12e0c25ec13f283d7b405a784051b497e3159"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:48.251723Z","signature_b64":"3DuFkyZL/e4soxdubDOrRqdQn0iVpI19Fv+ogQ1Si/LqTweo9f0ASP8HVWJfu0pdehljHvvc8fhWCI/bfvUKDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3309ea294a846d4d53b6954ec2f37d5d832dea070d0ea2a5412a41ba865ab904","last_reissued_at":"2026-05-18T00:26:48.251131Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:48.251131Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Investigation of the spin-1 honeycomb antiferromagnet BaNi$_2$V$_2$O$_8$ with easy plane anisotropy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Schneidewind, A. T. M. N. Islam, B. Klemke, B. Lake, E. A. Goremychkin, E. S. Klyushina, J. T. Park, M. M{\\aa}nsson, T. Guidi","submitted_at":"2018-01-03T11:31:58Z","abstract_excerpt":"The magnetic properties of the two-dimensional, S=1 honeycomb antiferromagnet BaNi$_2$V$_2$O$_8$ have been comprehensively studied using DC susceptibility measurements and inelastic neutron scattering techniques. The magnetic excitation spectrum is found to be dispersionless within experimental resolution between the honeycomb layers, while it disperses strongly within the honeycomb plane where it consists of two gapped spin-wave modes. The magnetic excitations are compared to linear spin-wave theory allowing the Hamiltonian to be determined. The first- and second-neighbour magnetic exchange i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.00962","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":""},"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":"1801.00962","created_at":"2026-05-18T00:26:48.251222+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.00962v1","created_at":"2026-05-18T00:26:48.251222+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.00962","created_at":"2026-05-18T00:26:48.251222+00:00"},{"alias_kind":"pith_short_12","alias_value":"GME6UKKKQRWU","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_16","alias_value":"GME6UKKKQRWU2U5W","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_8","alias_value":"GME6UKKK","created_at":"2026-05-18T12:32:25.280505+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/GME6UKKKQRWU2U5WSVHMF435LW","json":"https://pith.science/pith/GME6UKKKQRWU2U5WSVHMF435LW.json","graph_json":"https://pith.science/api/pith-number/GME6UKKKQRWU2U5WSVHMF435LW/graph.json","events_json":"https://pith.science/api/pith-number/GME6UKKKQRWU2U5WSVHMF435LW/events.json","paper":"https://pith.science/paper/GME6UKKK"},"agent_actions":{"view_html":"https://pith.science/pith/GME6UKKKQRWU2U5WSVHMF435LW","download_json":"https://pith.science/pith/GME6UKKKQRWU2U5WSVHMF435LW.json","view_paper":"https://pith.science/paper/GME6UKKK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.00962&json=true","fetch_graph":"https://pith.science/api/pith-number/GME6UKKKQRWU2U5WSVHMF435LW/graph.json","fetch_events":"https://pith.science/api/pith-number/GME6UKKKQRWU2U5WSVHMF435LW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GME6UKKKQRWU2U5WSVHMF435LW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GME6UKKKQRWU2U5WSVHMF435LW/action/storage_attestation","attest_author":"https://pith.science/pith/GME6UKKKQRWU2U5WSVHMF435LW/action/author_attestation","sign_citation":"https://pith.science/pith/GME6UKKKQRWU2U5WSVHMF435LW/action/citation_signature","submit_replication":"https://pith.science/pith/GME6UKKKQRWU2U5WSVHMF435LW/action/replication_record"}},"created_at":"2026-05-18T00:26:48.251222+00:00","updated_at":"2026-05-18T00:26:48.251222+00:00"}