{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:EEU6MWD3ZLY5MUDQ5WCKNQCI3K","short_pith_number":"pith:EEU6MWD3","schema_version":"1.0","canonical_sha256":"2129e6587bcaf1d65070ed84a6c048dab443f3160db22634be777351703d2261","source":{"kind":"arxiv","id":"1903.11675","version":1},"attestation_state":"computed","paper":{"title":"Theory of standing spin waves in finite-size chiral spin soliton lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A.S. Ovchinnikov, F. J. T. Goncalves, I.G. Bostrem, Igor Proskurin, J. Kishine, Vl.E. Sinitsyn, Y. Togawa","submitted_at":"2019-03-27T19:52:06Z","abstract_excerpt":"We present a theory of standing spin wave (SSW) in a monoaxial chiral helimagnet. Motivated by experimental findings on the magnetic field-dependence of the resonance frequency in thin films of Cr${}$Nb$_{3} $S${}_{6}$[Goncalves et al., Phys. Rev. B95, 104415 (2017)], we examine the SSW over a chiral soliton lattice (CSL) excited by an ac magnetic field applied parallel and perpendicular to the chiral axis. For this purpose, we generalize Kittel-Pincus theories of the SSW in ferromagnetic thin films to the case of non-collinear helimagnet with the surface end spins which are softly pinned by a"},"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":"1903.11675","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2019-03-27T19:52:06Z","cross_cats_sorted":[],"title_canon_sha256":"4a76b4e60f7a610b74c5109279b02013960183f87c1d3232a10745faaf08e641","abstract_canon_sha256":"a70a9236d579ce9f55780aaa804de416e91dcc6267141884ba0f685ed756382f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:40:32.906480Z","signature_b64":"unhisLrXuY9MzZxJ7VjJmYVzXbsqkxorgDQ4RqnuU0XWLI2U89BNKqlNwyf98UvYCwBbGOqKRaUKPegRzZ4wDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2129e6587bcaf1d65070ed84a6c048dab443f3160db22634be777351703d2261","last_reissued_at":"2026-05-17T23:40:32.905984Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:40:32.905984Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Theory of standing spin waves in finite-size chiral spin soliton lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A.S. Ovchinnikov, F. J. T. Goncalves, I.G. Bostrem, Igor Proskurin, J. Kishine, Vl.E. Sinitsyn, Y. Togawa","submitted_at":"2019-03-27T19:52:06Z","abstract_excerpt":"We present a theory of standing spin wave (SSW) in a monoaxial chiral helimagnet. Motivated by experimental findings on the magnetic field-dependence of the resonance frequency in thin films of Cr${}$Nb$_{3} $S${}_{6}$[Goncalves et al., Phys. Rev. B95, 104415 (2017)], we examine the SSW over a chiral soliton lattice (CSL) excited by an ac magnetic field applied parallel and perpendicular to the chiral axis. For this purpose, we generalize Kittel-Pincus theories of the SSW in ferromagnetic thin films to the case of non-collinear helimagnet with the surface end spins which are softly pinned by a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1903.11675","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":"1903.11675","created_at":"2026-05-17T23:40:32.906057+00:00"},{"alias_kind":"arxiv_version","alias_value":"1903.11675v1","created_at":"2026-05-17T23:40:32.906057+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1903.11675","created_at":"2026-05-17T23:40:32.906057+00:00"},{"alias_kind":"pith_short_12","alias_value":"EEU6MWD3ZLY5","created_at":"2026-05-18T12:33:15.570797+00:00"},{"alias_kind":"pith_short_16","alias_value":"EEU6MWD3ZLY5MUDQ","created_at":"2026-05-18T12:33:15.570797+00:00"},{"alias_kind":"pith_short_8","alias_value":"EEU6MWD3","created_at":"2026-05-18T12:33:15.570797+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/EEU6MWD3ZLY5MUDQ5WCKNQCI3K","json":"https://pith.science/pith/EEU6MWD3ZLY5MUDQ5WCKNQCI3K.json","graph_json":"https://pith.science/api/pith-number/EEU6MWD3ZLY5MUDQ5WCKNQCI3K/graph.json","events_json":"https://pith.science/api/pith-number/EEU6MWD3ZLY5MUDQ5WCKNQCI3K/events.json","paper":"https://pith.science/paper/EEU6MWD3"},"agent_actions":{"view_html":"https://pith.science/pith/EEU6MWD3ZLY5MUDQ5WCKNQCI3K","download_json":"https://pith.science/pith/EEU6MWD3ZLY5MUDQ5WCKNQCI3K.json","view_paper":"https://pith.science/paper/EEU6MWD3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1903.11675&json=true","fetch_graph":"https://pith.science/api/pith-number/EEU6MWD3ZLY5MUDQ5WCKNQCI3K/graph.json","fetch_events":"https://pith.science/api/pith-number/EEU6MWD3ZLY5MUDQ5WCKNQCI3K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EEU6MWD3ZLY5MUDQ5WCKNQCI3K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EEU6MWD3ZLY5MUDQ5WCKNQCI3K/action/storage_attestation","attest_author":"https://pith.science/pith/EEU6MWD3ZLY5MUDQ5WCKNQCI3K/action/author_attestation","sign_citation":"https://pith.science/pith/EEU6MWD3ZLY5MUDQ5WCKNQCI3K/action/citation_signature","submit_replication":"https://pith.science/pith/EEU6MWD3ZLY5MUDQ5WCKNQCI3K/action/replication_record"}},"created_at":"2026-05-17T23:40:32.906057+00:00","updated_at":"2026-05-17T23:40:32.906057+00:00"}