{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:LZTCSOIOGQUJYKTSQKNNXDSIMY","short_pith_number":"pith:LZTCSOIO","schema_version":"1.0","canonical_sha256":"5e6629390e34289c2a72829adb8e48661668eac37ffa31933e614a2b58332eea","source":{"kind":"arxiv","id":"0912.3650","version":1},"attestation_state":"computed","paper":{"title":"Oscillatory transient regime in the forced dynamics of a spin torque nano-oscillator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Andrei Slavin, Ezio Iacocca, Johan Akerman, Vasil Tiberkevich, Yan Zhou","submitted_at":"2009-12-18T11:41:12Z","abstract_excerpt":"We demonstrate that the transient non-autonomous dynamics of a spin torque nano-oscillator (STNO) under a radio-frequency (rf) driving signal is qualitatively different from the dynamics described by the Adler model. If the external rf current $I_{rf}$ is larger than a certain critical value $I_{cr}$ (determined by the STNO bias current and damping) strong oscillations of the STNO power and phase develop in the transient regime. The frequency of these oscillations increases with $I_{rf}$ as $\\propto\\sqrt{I_{rf} - I_{cr}}$ and can reach several GHz, whereas the damping rate of the oscillations "},"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":"0912.3650","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-12-18T11:41:12Z","cross_cats_sorted":[],"title_canon_sha256":"63fff0dd93deedd31721abea3b7d7cbee12d56f588db38157a0c1221272b6593","abstract_canon_sha256":"60ab79d31ed6a421e2cf9223ab47bbaea2f38171c02ee73e7e7a3a39d09d48ab"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:10:15.649489Z","signature_b64":"+wg3QSrKMQZnxQJcEHwJ8RC+4HMH3JdkqGtVTCY2z3SGyuLVnYx53xM9NalWeklVFdaJo/ke13N4BbZMmqRrAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e6629390e34289c2a72829adb8e48661668eac37ffa31933e614a2b58332eea","last_reissued_at":"2026-05-18T02:10:15.648833Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:10:15.648833Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Oscillatory transient regime in the forced dynamics of a spin torque nano-oscillator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Andrei Slavin, Ezio Iacocca, Johan Akerman, Vasil Tiberkevich, Yan Zhou","submitted_at":"2009-12-18T11:41:12Z","abstract_excerpt":"We demonstrate that the transient non-autonomous dynamics of a spin torque nano-oscillator (STNO) under a radio-frequency (rf) driving signal is qualitatively different from the dynamics described by the Adler model. If the external rf current $I_{rf}$ is larger than a certain critical value $I_{cr}$ (determined by the STNO bias current and damping) strong oscillations of the STNO power and phase develop in the transient regime. The frequency of these oscillations increases with $I_{rf}$ as $\\propto\\sqrt{I_{rf} - I_{cr}}$ and can reach several GHz, whereas the damping rate of the oscillations "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0912.3650","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":"0912.3650","created_at":"2026-05-18T02:10:15.648916+00:00"},{"alias_kind":"arxiv_version","alias_value":"0912.3650v1","created_at":"2026-05-18T02:10:15.648916+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0912.3650","created_at":"2026-05-18T02:10:15.648916+00:00"},{"alias_kind":"pith_short_12","alias_value":"LZTCSOIOGQUJ","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_16","alias_value":"LZTCSOIOGQUJYKTS","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_8","alias_value":"LZTCSOIO","created_at":"2026-05-18T12:26:00.592388+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/LZTCSOIOGQUJYKTSQKNNXDSIMY","json":"https://pith.science/pith/LZTCSOIOGQUJYKTSQKNNXDSIMY.json","graph_json":"https://pith.science/api/pith-number/LZTCSOIOGQUJYKTSQKNNXDSIMY/graph.json","events_json":"https://pith.science/api/pith-number/LZTCSOIOGQUJYKTSQKNNXDSIMY/events.json","paper":"https://pith.science/paper/LZTCSOIO"},"agent_actions":{"view_html":"https://pith.science/pith/LZTCSOIOGQUJYKTSQKNNXDSIMY","download_json":"https://pith.science/pith/LZTCSOIOGQUJYKTSQKNNXDSIMY.json","view_paper":"https://pith.science/paper/LZTCSOIO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0912.3650&json=true","fetch_graph":"https://pith.science/api/pith-number/LZTCSOIOGQUJYKTSQKNNXDSIMY/graph.json","fetch_events":"https://pith.science/api/pith-number/LZTCSOIOGQUJYKTSQKNNXDSIMY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LZTCSOIOGQUJYKTSQKNNXDSIMY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LZTCSOIOGQUJYKTSQKNNXDSIMY/action/storage_attestation","attest_author":"https://pith.science/pith/LZTCSOIOGQUJYKTSQKNNXDSIMY/action/author_attestation","sign_citation":"https://pith.science/pith/LZTCSOIOGQUJYKTSQKNNXDSIMY/action/citation_signature","submit_replication":"https://pith.science/pith/LZTCSOIOGQUJYKTSQKNNXDSIMY/action/replication_record"}},"created_at":"2026-05-18T02:10:15.648916+00:00","updated_at":"2026-05-18T02:10:15.648916+00:00"}