{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:S5STP3A2EAOWKM4ZXEPDSOOGXJ","short_pith_number":"pith:S5STP3A2","schema_version":"1.0","canonical_sha256":"976537ec1a201d653399b91e3939c6ba4dc1ac3064dd985bceddb5a258dc542b","source":{"kind":"arxiv","id":"1703.04430","version":2},"attestation_state":"computed","paper":{"title":"Field dependence of the magnetic correlations of the frustrated magnet SrDy$_2$O$_4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A.D. Bianchi, A. D\\'esilets-Benoit, A. Fennell, B. Pr\\'evost, H.A. Dabkowska, M. Frontzek, M. Kenzelmann, N. Gauthier, O. Zaharko, R. Sibille","submitted_at":"2017-03-13T14:56:08Z","abstract_excerpt":"The frustrated magnet SrDy$_2$O$_4$ exhibits a field-induced phase with a magnetization plateau at $1/3$ of the saturation value for magnetic fields applied along the $b$-axis. We report here a neutron scattering study of the nature and symmetry of the magnetic order in this field-induced phase. Below $T\\approx 0.5$ K, there are strong hysteretic effects, and the order is short or long ranged for zero-field and field cooling, respectively. We find that the long-range ordered magnetic structure within the zig-zag chains is identical to that expected for the one-dimensional axial next-nearest ne"},"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":"1703.04430","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-03-13T14:56:08Z","cross_cats_sorted":[],"title_canon_sha256":"0cd5c2402349d01e7b79400a20cb5fd9abb70e75d14c594ab34d4fb46375bbad","abstract_canon_sha256":"89bc89b5dff213c5a2398d3c2d24028b450e55aac41870f97d7c7527045b5daf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:43:20.559857Z","signature_b64":"ZprzzocmhTOCYZX1DFqgRYG9y4VPJ5Az8PDxKcydieLk2bxHYanjvG14lLI0fCxr2LGHb0YDDjudrxPa9eTPDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"976537ec1a201d653399b91e3939c6ba4dc1ac3064dd985bceddb5a258dc542b","last_reissued_at":"2026-05-18T00:43:20.559257Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:43:20.559257Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Field dependence of the magnetic correlations of the frustrated magnet SrDy$_2$O$_4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A.D. Bianchi, A. D\\'esilets-Benoit, A. Fennell, B. Pr\\'evost, H.A. Dabkowska, M. Frontzek, M. Kenzelmann, N. Gauthier, O. Zaharko, R. Sibille","submitted_at":"2017-03-13T14:56:08Z","abstract_excerpt":"The frustrated magnet SrDy$_2$O$_4$ exhibits a field-induced phase with a magnetization plateau at $1/3$ of the saturation value for magnetic fields applied along the $b$-axis. We report here a neutron scattering study of the nature and symmetry of the magnetic order in this field-induced phase. Below $T\\approx 0.5$ K, there are strong hysteretic effects, and the order is short or long ranged for zero-field and field cooling, respectively. We find that the long-range ordered magnetic structure within the zig-zag chains is identical to that expected for the one-dimensional axial next-nearest ne"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.04430","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":"1703.04430","created_at":"2026-05-18T00:43:20.559347+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.04430v2","created_at":"2026-05-18T00:43:20.559347+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.04430","created_at":"2026-05-18T00:43:20.559347+00:00"},{"alias_kind":"pith_short_12","alias_value":"S5STP3A2EAOW","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_16","alias_value":"S5STP3A2EAOWKM4Z","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_8","alias_value":"S5STP3A2","created_at":"2026-05-18T12:31:43.269735+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/S5STP3A2EAOWKM4ZXEPDSOOGXJ","json":"https://pith.science/pith/S5STP3A2EAOWKM4ZXEPDSOOGXJ.json","graph_json":"https://pith.science/api/pith-number/S5STP3A2EAOWKM4ZXEPDSOOGXJ/graph.json","events_json":"https://pith.science/api/pith-number/S5STP3A2EAOWKM4ZXEPDSOOGXJ/events.json","paper":"https://pith.science/paper/S5STP3A2"},"agent_actions":{"view_html":"https://pith.science/pith/S5STP3A2EAOWKM4ZXEPDSOOGXJ","download_json":"https://pith.science/pith/S5STP3A2EAOWKM4ZXEPDSOOGXJ.json","view_paper":"https://pith.science/paper/S5STP3A2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.04430&json=true","fetch_graph":"https://pith.science/api/pith-number/S5STP3A2EAOWKM4ZXEPDSOOGXJ/graph.json","fetch_events":"https://pith.science/api/pith-number/S5STP3A2EAOWKM4ZXEPDSOOGXJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/S5STP3A2EAOWKM4ZXEPDSOOGXJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/S5STP3A2EAOWKM4ZXEPDSOOGXJ/action/storage_attestation","attest_author":"https://pith.science/pith/S5STP3A2EAOWKM4ZXEPDSOOGXJ/action/author_attestation","sign_citation":"https://pith.science/pith/S5STP3A2EAOWKM4ZXEPDSOOGXJ/action/citation_signature","submit_replication":"https://pith.science/pith/S5STP3A2EAOWKM4ZXEPDSOOGXJ/action/replication_record"}},"created_at":"2026-05-18T00:43:20.559347+00:00","updated_at":"2026-05-18T00:43:20.559347+00:00"}