{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:4T7OOUHEHAN6DHEWKRMLI6FLKZ","short_pith_number":"pith:4T7OOUHE","schema_version":"1.0","canonical_sha256":"e4fee750e4381be19c965458b478ab566f4b9d051e49d6044ebf155ce8bc95ff","source":{"kind":"arxiv","id":"1507.02593","version":2},"attestation_state":"computed","paper":{"title":"Temperature evolution of superparamagnetic clusters in single-crystal La0.85Sr0.15CoO3 from nonlinear magnetic ac response and neutron depolarization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A. V. Lazuta, V. A. Ryzhov, V. P. Khavronin, V. V. Deriglazov, V. V. Runov","submitted_at":"2015-07-09T16:53:39Z","abstract_excerpt":"The representative measurements of the second harmonic in ac magnetization complemented by neutron depolarization have been performed for single-crystal La0.85Sr0.15CoO3 in the temperature range 97 K < T < 230 K, where occurrence of a small fraction (~ 0.001) of nanoscale ferromagnetic clusters (FMC) has been found. Magnetic, geometrical and dynamical parameters of the FMC system have been evaluated in the temperature range T < 140 K, where superparamagnetic regime installs, by means of the formalism involving the Fokker-Planck equation (FPE). With lowering the temperature, the amount of clust"},"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":"1507.02593","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2015-07-09T16:53:39Z","cross_cats_sorted":[],"title_canon_sha256":"d1eca2dede2b4859d8f93065fb5b719993511f221db198840e3c56a3b41c151a","abstract_canon_sha256":"fa719dac05b2a2553513e6517a17fc131c69342a2a40d66d3d9f78b80a6f7a78"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:30:23.746378Z","signature_b64":"h03/Fd2sh2C4KSsgkV1Ngygn4PHozX+xWoChcsuccaIp+EJYqx3HQ9l4hMRZ1sJxjog45gbOy4W/G2Jzjk2BAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e4fee750e4381be19c965458b478ab566f4b9d051e49d6044ebf155ce8bc95ff","last_reissued_at":"2026-05-18T01:30:23.745663Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:30:23.745663Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Temperature evolution of superparamagnetic clusters in single-crystal La0.85Sr0.15CoO3 from nonlinear magnetic ac response and neutron depolarization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A. V. Lazuta, V. A. Ryzhov, V. P. Khavronin, V. V. Deriglazov, V. V. Runov","submitted_at":"2015-07-09T16:53:39Z","abstract_excerpt":"The representative measurements of the second harmonic in ac magnetization complemented by neutron depolarization have been performed for single-crystal La0.85Sr0.15CoO3 in the temperature range 97 K < T < 230 K, where occurrence of a small fraction (~ 0.001) of nanoscale ferromagnetic clusters (FMC) has been found. Magnetic, geometrical and dynamical parameters of the FMC system have been evaluated in the temperature range T < 140 K, where superparamagnetic regime installs, by means of the formalism involving the Fokker-Planck equation (FPE). With lowering the temperature, the amount of clust"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.02593","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":"1507.02593","created_at":"2026-05-18T01:30:23.745773+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.02593v2","created_at":"2026-05-18T01:30:23.745773+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.02593","created_at":"2026-05-18T01:30:23.745773+00:00"},{"alias_kind":"pith_short_12","alias_value":"4T7OOUHEHAN6","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_16","alias_value":"4T7OOUHEHAN6DHEW","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_8","alias_value":"4T7OOUHE","created_at":"2026-05-18T12:29:05.191682+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/4T7OOUHEHAN6DHEWKRMLI6FLKZ","json":"https://pith.science/pith/4T7OOUHEHAN6DHEWKRMLI6FLKZ.json","graph_json":"https://pith.science/api/pith-number/4T7OOUHEHAN6DHEWKRMLI6FLKZ/graph.json","events_json":"https://pith.science/api/pith-number/4T7OOUHEHAN6DHEWKRMLI6FLKZ/events.json","paper":"https://pith.science/paper/4T7OOUHE"},"agent_actions":{"view_html":"https://pith.science/pith/4T7OOUHEHAN6DHEWKRMLI6FLKZ","download_json":"https://pith.science/pith/4T7OOUHEHAN6DHEWKRMLI6FLKZ.json","view_paper":"https://pith.science/paper/4T7OOUHE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.02593&json=true","fetch_graph":"https://pith.science/api/pith-number/4T7OOUHEHAN6DHEWKRMLI6FLKZ/graph.json","fetch_events":"https://pith.science/api/pith-number/4T7OOUHEHAN6DHEWKRMLI6FLKZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4T7OOUHEHAN6DHEWKRMLI6FLKZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4T7OOUHEHAN6DHEWKRMLI6FLKZ/action/storage_attestation","attest_author":"https://pith.science/pith/4T7OOUHEHAN6DHEWKRMLI6FLKZ/action/author_attestation","sign_citation":"https://pith.science/pith/4T7OOUHEHAN6DHEWKRMLI6FLKZ/action/citation_signature","submit_replication":"https://pith.science/pith/4T7OOUHEHAN6DHEWKRMLI6FLKZ/action/replication_record"}},"created_at":"2026-05-18T01:30:23.745773+00:00","updated_at":"2026-05-18T01:30:23.745773+00:00"}