{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:NCYASCPRH4F5N6KIITQ45PCVVF","short_pith_number":"pith:NCYASCPR","schema_version":"1.0","canonical_sha256":"68b00909f13f0bd6f94844e1cebc55a9682b68fafb2e6d020067e4bee60a6421","source":{"kind":"arxiv","id":"1703.01879","version":5},"attestation_state":"computed","paper":{"title":"Damping dependence of spin-torque effects in thermally assisted magnetization reversal","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"D. Byrne, J.E. Wegrowe, S.V.Titov, W. J. Dowling, W.T. Coffey, Y.P. Kalmykov","submitted_at":"2017-03-06T14:07:12Z","abstract_excerpt":"Thermal fluctuations of nanomagnets driven by spin-polarized currents are treated via the Landau-Lifshitz-Gilbert equation as generalized to include both the random thermal noise field and Slonczewski spin-transfer torque terms. The magnetization reversal time of such a nanomagnet is then evaluated for wide ranges of damping by using a method which generalizes the solution of the so-called Kramers turnover problem for mechanical Brownian particles, thereby bridging the very low damping and intermediate damping Kramers escape rates, to the analogous magnetic turnover problem. The reversal time "},"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":"1703.01879","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-06T14:07:12Z","cross_cats_sorted":[],"title_canon_sha256":"ef8025a90e64fc2673213ec98854daa9aa89052efcb8f954b0f6ed68f83f1685","abstract_canon_sha256":"f76effa65e17e2390150f3351c5dfff6460213cd13304a4dddb2b4a37a79937a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:34:31.140602Z","signature_b64":"ATF+I4r1Cgf8x0R9vTYH4YDxlsrJmLl1xYlAKbpGyCAFNIhxYLf2YcUB15VXqJBZsmS4QTzj8lYm/e9Qx7cDBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"68b00909f13f0bd6f94844e1cebc55a9682b68fafb2e6d020067e4bee60a6421","last_reissued_at":"2026-05-18T00:34:31.140212Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:34:31.140212Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Damping dependence of spin-torque effects in thermally assisted magnetization reversal","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"D. Byrne, J.E. Wegrowe, S.V.Titov, W. J. Dowling, W.T. Coffey, Y.P. Kalmykov","submitted_at":"2017-03-06T14:07:12Z","abstract_excerpt":"Thermal fluctuations of nanomagnets driven by spin-polarized currents are treated via the Landau-Lifshitz-Gilbert equation as generalized to include both the random thermal noise field and Slonczewski spin-transfer torque terms. The magnetization reversal time of such a nanomagnet is then evaluated for wide ranges of damping by using a method which generalizes the solution of the so-called Kramers turnover problem for mechanical Brownian particles, thereby bridging the very low damping and intermediate damping Kramers escape rates, to the analogous magnetic turnover problem. The reversal time "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.01879","kind":"arxiv","version":5},"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":"1703.01879","created_at":"2026-05-18T00:34:31.140264+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.01879v5","created_at":"2026-05-18T00:34:31.140264+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.01879","created_at":"2026-05-18T00:34:31.140264+00:00"},{"alias_kind":"pith_short_12","alias_value":"NCYASCPRH4F5","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_16","alias_value":"NCYASCPRH4F5N6KI","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_8","alias_value":"NCYASCPR","created_at":"2026-05-18T12:31:31.346846+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/NCYASCPRH4F5N6KIITQ45PCVVF","json":"https://pith.science/pith/NCYASCPRH4F5N6KIITQ45PCVVF.json","graph_json":"https://pith.science/api/pith-number/NCYASCPRH4F5N6KIITQ45PCVVF/graph.json","events_json":"https://pith.science/api/pith-number/NCYASCPRH4F5N6KIITQ45PCVVF/events.json","paper":"https://pith.science/paper/NCYASCPR"},"agent_actions":{"view_html":"https://pith.science/pith/NCYASCPRH4F5N6KIITQ45PCVVF","download_json":"https://pith.science/pith/NCYASCPRH4F5N6KIITQ45PCVVF.json","view_paper":"https://pith.science/paper/NCYASCPR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.01879&json=true","fetch_graph":"https://pith.science/api/pith-number/NCYASCPRH4F5N6KIITQ45PCVVF/graph.json","fetch_events":"https://pith.science/api/pith-number/NCYASCPRH4F5N6KIITQ45PCVVF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NCYASCPRH4F5N6KIITQ45PCVVF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NCYASCPRH4F5N6KIITQ45PCVVF/action/storage_attestation","attest_author":"https://pith.science/pith/NCYASCPRH4F5N6KIITQ45PCVVF/action/author_attestation","sign_citation":"https://pith.science/pith/NCYASCPRH4F5N6KIITQ45PCVVF/action/citation_signature","submit_replication":"https://pith.science/pith/NCYASCPRH4F5N6KIITQ45PCVVF/action/replication_record"}},"created_at":"2026-05-18T00:34:31.140264+00:00","updated_at":"2026-05-18T00:34:31.140264+00:00"}