{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:DRBVYWGWMX2NESDTDJY7BSHVVP","short_pith_number":"pith:DRBVYWGW","schema_version":"1.0","canonical_sha256":"1c435c58d665f4d248731a71f0c8f5abf0064f211705364c4bb4bcd5d9f889b5","source":{"kind":"arxiv","id":"1112.5077","version":1},"attestation_state":"computed","paper":{"title":"Vortex motion in Nb/PdNi/Nb trilayers: new aspects in the flux flow state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"C. Attanasio, C. Cirillo, E. A. Ilyina, E. Silva, K. Torokhtii, N. Pompeo, S. Sarti","submitted_at":"2011-12-21T16:12:52Z","abstract_excerpt":"We study the dynamics of vortex lines in Supercondutor/Ferromagnet/Superconductor (SFS) heterostructures at microwave frequencies. We have employed swept-frequency, Corbino-disk and resonant, dielectric-resonator techniques to obtain the field and temperature dependence of the vortex-state parameters. We concentrate here on the genuine flux-flow resistivity $\\rho_{ff}$, that we access at subcritical currents using a sufficiently high driving frequency. We find that $\\rho_{ff}$ does not follow the well-known Bardeen-Stephen model. Instead, it is well described by a full time-dependent Ginzburg-"},"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":"1112.5077","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-12-21T16:12:52Z","cross_cats_sorted":[],"title_canon_sha256":"1e25637e8ee16085416307eeb06b9dc2373806ca498ed90a5e4f68a4d65d98cb","abstract_canon_sha256":"1e1f8b0e506bb8a7f4212f0fdaee17ba35fd425bacfe6f0abf70856dc0f27c7c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:03.863476Z","signature_b64":"Xtk/+RKUIj7haXLsrZbwQhDO7Whwg+d1cH3zyNUikB2Nex7RX1QIlZoRBYX0lQjSOP/3XHR+HUIvqad4xSgABg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c435c58d665f4d248731a71f0c8f5abf0064f211705364c4bb4bcd5d9f889b5","last_reissued_at":"2026-05-18T01:59:03.862540Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:03.862540Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Vortex motion in Nb/PdNi/Nb trilayers: new aspects in the flux flow state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"C. Attanasio, C. Cirillo, E. A. Ilyina, E. Silva, K. Torokhtii, N. Pompeo, S. Sarti","submitted_at":"2011-12-21T16:12:52Z","abstract_excerpt":"We study the dynamics of vortex lines in Supercondutor/Ferromagnet/Superconductor (SFS) heterostructures at microwave frequencies. We have employed swept-frequency, Corbino-disk and resonant, dielectric-resonator techniques to obtain the field and temperature dependence of the vortex-state parameters. We concentrate here on the genuine flux-flow resistivity $\\rho_{ff}$, that we access at subcritical currents using a sufficiently high driving frequency. We find that $\\rho_{ff}$ does not follow the well-known Bardeen-Stephen model. Instead, it is well described by a full time-dependent Ginzburg-"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.5077","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":"1112.5077","created_at":"2026-05-18T01:59:03.862722+00:00"},{"alias_kind":"arxiv_version","alias_value":"1112.5077v1","created_at":"2026-05-18T01:59:03.862722+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.5077","created_at":"2026-05-18T01:59:03.862722+00:00"},{"alias_kind":"pith_short_12","alias_value":"DRBVYWGWMX2N","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_16","alias_value":"DRBVYWGWMX2NESDT","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_8","alias_value":"DRBVYWGW","created_at":"2026-05-18T12:26:26.731475+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/DRBVYWGWMX2NESDTDJY7BSHVVP","json":"https://pith.science/pith/DRBVYWGWMX2NESDTDJY7BSHVVP.json","graph_json":"https://pith.science/api/pith-number/DRBVYWGWMX2NESDTDJY7BSHVVP/graph.json","events_json":"https://pith.science/api/pith-number/DRBVYWGWMX2NESDTDJY7BSHVVP/events.json","paper":"https://pith.science/paper/DRBVYWGW"},"agent_actions":{"view_html":"https://pith.science/pith/DRBVYWGWMX2NESDTDJY7BSHVVP","download_json":"https://pith.science/pith/DRBVYWGWMX2NESDTDJY7BSHVVP.json","view_paper":"https://pith.science/paper/DRBVYWGW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1112.5077&json=true","fetch_graph":"https://pith.science/api/pith-number/DRBVYWGWMX2NESDTDJY7BSHVVP/graph.json","fetch_events":"https://pith.science/api/pith-number/DRBVYWGWMX2NESDTDJY7BSHVVP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DRBVYWGWMX2NESDTDJY7BSHVVP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DRBVYWGWMX2NESDTDJY7BSHVVP/action/storage_attestation","attest_author":"https://pith.science/pith/DRBVYWGWMX2NESDTDJY7BSHVVP/action/author_attestation","sign_citation":"https://pith.science/pith/DRBVYWGWMX2NESDTDJY7BSHVVP/action/citation_signature","submit_replication":"https://pith.science/pith/DRBVYWGWMX2NESDTDJY7BSHVVP/action/replication_record"}},"created_at":"2026-05-18T01:59:03.862722+00:00","updated_at":"2026-05-18T01:59:03.862722+00:00"}