{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:PR2Z4BHG77K2YYEVWSFL255Q63","short_pith_number":"pith:PR2Z4BHG","schema_version":"1.0","canonical_sha256":"7c759e04e6ffd5ac6095b48abd77b0f6d720b12fae35b71159a19a109d8bc064","source":{"kind":"arxiv","id":"2208.09368","version":1},"attestation_state":"computed","paper":{"title":"The magnetic structure and field dependence of the cycloid phase mediating the spin reorientation transition in Ca$_3$Ru$_2$O$_7$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"C. D. Dashwood, C. V. Colin, D. F. McMorrow, E. Ressouche, G. B. G. Stenning, J. Spratt, Q. Faure, R. D. Johnson, R. S. Perry","submitted_at":"2022-08-19T14:30:41Z","abstract_excerpt":"We report a comprehensive experimental investigation of the magnetic structure of the cycloidal phase in Ca$_3$Ru$_2$O$_7$, which mediates the spin reorientation transition, and establishes its magnetic phase diagram. In zero applied field, single-crystal neutron diffraction data confirms the scenario deduced from an earlier resonant x-ray scattering study: between $46.7$~K $< T < 49.0$~K the magnetic moments form a cycloid in the $a-b$ plane with a propagation wavevector of $(\\delta,0,1)$ with $\\delta \\simeq 0.025$ and an ordered moment of about 1 $\\mu_{\\rm{B}}$, with the eccentricity of the "},"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":"2208.09368","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-08-19T14:30:41Z","cross_cats_sorted":[],"title_canon_sha256":"210ace4ee7ace0f63f169fce340150e43d61a4a8fa3c2237c5d6bdf6ea3dd9d3","abstract_canon_sha256":"c71f219da9afffd8649a48a13049f4fe288f630d6298e393c5c61ef0363404fc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:49:59.223480Z","signature_b64":"p9LLy5ZJnQ6FLVuWJygkejyb/XWace111G1IXQojPeKvXh23KtQSuTzBDHxG2gdso4S44FFlO0Xip2wBlBw8CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7c759e04e6ffd5ac6095b48abd77b0f6d720b12fae35b71159a19a109d8bc064","last_reissued_at":"2026-07-05T04:49:59.223045Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:49:59.223045Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The magnetic structure and field dependence of the cycloid phase mediating the spin reorientation transition in Ca$_3$Ru$_2$O$_7$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"C. D. Dashwood, C. V. Colin, D. F. McMorrow, E. Ressouche, G. B. G. Stenning, J. Spratt, Q. Faure, R. D. Johnson, R. S. Perry","submitted_at":"2022-08-19T14:30:41Z","abstract_excerpt":"We report a comprehensive experimental investigation of the magnetic structure of the cycloidal phase in Ca$_3$Ru$_2$O$_7$, which mediates the spin reorientation transition, and establishes its magnetic phase diagram. In zero applied field, single-crystal neutron diffraction data confirms the scenario deduced from an earlier resonant x-ray scattering study: between $46.7$~K $< T < 49.0$~K the magnetic moments form a cycloid in the $a-b$ plane with a propagation wavevector of $(\\delta,0,1)$ with $\\delta \\simeq 0.025$ and an ordered moment of about 1 $\\mu_{\\rm{B}}$, with the eccentricity of the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.09368","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/2208.09368/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":"2208.09368","created_at":"2026-07-05T04:49:59.223099+00:00"},{"alias_kind":"arxiv_version","alias_value":"2208.09368v1","created_at":"2026-07-05T04:49:59.223099+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.09368","created_at":"2026-07-05T04:49:59.223099+00:00"},{"alias_kind":"pith_short_12","alias_value":"PR2Z4BHG77K2","created_at":"2026-07-05T04:49:59.223099+00:00"},{"alias_kind":"pith_short_16","alias_value":"PR2Z4BHG77K2YYEV","created_at":"2026-07-05T04:49:59.223099+00:00"},{"alias_kind":"pith_short_8","alias_value":"PR2Z4BHG","created_at":"2026-07-05T04:49:59.223099+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/PR2Z4BHG77K2YYEVWSFL255Q63","json":"https://pith.science/pith/PR2Z4BHG77K2YYEVWSFL255Q63.json","graph_json":"https://pith.science/api/pith-number/PR2Z4BHG77K2YYEVWSFL255Q63/graph.json","events_json":"https://pith.science/api/pith-number/PR2Z4BHG77K2YYEVWSFL255Q63/events.json","paper":"https://pith.science/paper/PR2Z4BHG"},"agent_actions":{"view_html":"https://pith.science/pith/PR2Z4BHG77K2YYEVWSFL255Q63","download_json":"https://pith.science/pith/PR2Z4BHG77K2YYEVWSFL255Q63.json","view_paper":"https://pith.science/paper/PR2Z4BHG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2208.09368&json=true","fetch_graph":"https://pith.science/api/pith-number/PR2Z4BHG77K2YYEVWSFL255Q63/graph.json","fetch_events":"https://pith.science/api/pith-number/PR2Z4BHG77K2YYEVWSFL255Q63/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PR2Z4BHG77K2YYEVWSFL255Q63/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PR2Z4BHG77K2YYEVWSFL255Q63/action/storage_attestation","attest_author":"https://pith.science/pith/PR2Z4BHG77K2YYEVWSFL255Q63/action/author_attestation","sign_citation":"https://pith.science/pith/PR2Z4BHG77K2YYEVWSFL255Q63/action/citation_signature","submit_replication":"https://pith.science/pith/PR2Z4BHG77K2YYEVWSFL255Q63/action/replication_record"}},"created_at":"2026-07-05T04:49:59.223099+00:00","updated_at":"2026-07-05T04:49:59.223099+00:00"}