{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:FC4BHC234GXS6LNNGAAZXYSXDD","short_pith_number":"pith:FC4BHC23","schema_version":"1.0","canonical_sha256":"28b8138b5be1af2f2dad30019be25718ebd6ec933bfe65a1622b31a6ca249d2a","source":{"kind":"arxiv","id":"2505.24659","version":1},"attestation_state":"computed","paper":{"title":"Magnetoimpedance properties of CoNbZr, multilayer CoNbZr/Au and multilayer NiFe/Au thin films","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.app-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Indujan Sivanesarajah, Leon Abelmann, Uwe Hartmann","submitted_at":"2025-05-30T14:46:29Z","abstract_excerpt":"Thin-film magnetic sensors using the giant magnetoimpedance (GMI) effect show great promise for sensitive low-field magnetic measurements. Optimising sensor performance requires a thorough understanding of the properties of various soft magnetic materials. This study examines the electric, magnetic, and GMI properties of sputtered single-layer amorphous CoNbZr, multilayer amorphous CoNbZr/Au, and crystalline NiFe/Au thin films. GMI measurements reveal distinct ferromagnetic resonance (FMR) frequencies: 1.4 GHz for CoNbZr, 0.7 GHz for CoNbZr/Au, and 0.5 GHz for NiFe/Au. Au interlayers improve t"},"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":"2505.24659","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-05-30T14:46:29Z","cross_cats_sorted":["physics.app-ph"],"title_canon_sha256":"274f0ba97d96b408eb9156d9dd295c3ae463f0a911c03dbc193567c45345b071","abstract_canon_sha256":"8f15111c71c95e5c6d205cd45775a523e7dff37f469df8b9d8b2f2540d2acc72"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:12:54.167572Z","signature_b64":"pU9gydS20CJOvjZuBD6ylh1cw1NUjSErKlJmckI39C5IILuYo6H74zqi25wlGad8C++wRiLSDXxJBrjEc0w1BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"28b8138b5be1af2f2dad30019be25718ebd6ec933bfe65a1622b31a6ca249d2a","last_reissued_at":"2026-07-05T11:12:54.167085Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:12:54.167085Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetoimpedance properties of CoNbZr, multilayer CoNbZr/Au and multilayer NiFe/Au thin films","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.app-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Indujan Sivanesarajah, Leon Abelmann, Uwe Hartmann","submitted_at":"2025-05-30T14:46:29Z","abstract_excerpt":"Thin-film magnetic sensors using the giant magnetoimpedance (GMI) effect show great promise for sensitive low-field magnetic measurements. Optimising sensor performance requires a thorough understanding of the properties of various soft magnetic materials. This study examines the electric, magnetic, and GMI properties of sputtered single-layer amorphous CoNbZr, multilayer amorphous CoNbZr/Au, and crystalline NiFe/Au thin films. GMI measurements reveal distinct ferromagnetic resonance (FMR) frequencies: 1.4 GHz for CoNbZr, 0.7 GHz for CoNbZr/Au, and 0.5 GHz for NiFe/Au. Au interlayers improve t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.24659","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.24659/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2505.24659","created_at":"2026-07-05T11:12:54.167148+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.24659v1","created_at":"2026-07-05T11:12:54.167148+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.24659","created_at":"2026-07-05T11:12:54.167148+00:00"},{"alias_kind":"pith_short_12","alias_value":"FC4BHC234GXS","created_at":"2026-07-05T11:12:54.167148+00:00"},{"alias_kind":"pith_short_16","alias_value":"FC4BHC234GXS6LNN","created_at":"2026-07-05T11:12:54.167148+00:00"},{"alias_kind":"pith_short_8","alias_value":"FC4BHC23","created_at":"2026-07-05T11:12:54.167148+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/FC4BHC234GXS6LNNGAAZXYSXDD","json":"https://pith.science/pith/FC4BHC234GXS6LNNGAAZXYSXDD.json","graph_json":"https://pith.science/api/pith-number/FC4BHC234GXS6LNNGAAZXYSXDD/graph.json","events_json":"https://pith.science/api/pith-number/FC4BHC234GXS6LNNGAAZXYSXDD/events.json","paper":"https://pith.science/paper/FC4BHC23"},"agent_actions":{"view_html":"https://pith.science/pith/FC4BHC234GXS6LNNGAAZXYSXDD","download_json":"https://pith.science/pith/FC4BHC234GXS6LNNGAAZXYSXDD.json","view_paper":"https://pith.science/paper/FC4BHC23","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.24659&json=true","fetch_graph":"https://pith.science/api/pith-number/FC4BHC234GXS6LNNGAAZXYSXDD/graph.json","fetch_events":"https://pith.science/api/pith-number/FC4BHC234GXS6LNNGAAZXYSXDD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FC4BHC234GXS6LNNGAAZXYSXDD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FC4BHC234GXS6LNNGAAZXYSXDD/action/storage_attestation","attest_author":"https://pith.science/pith/FC4BHC234GXS6LNNGAAZXYSXDD/action/author_attestation","sign_citation":"https://pith.science/pith/FC4BHC234GXS6LNNGAAZXYSXDD/action/citation_signature","submit_replication":"https://pith.science/pith/FC4BHC234GXS6LNNGAAZXYSXDD/action/replication_record"}},"created_at":"2026-07-05T11:12:54.167148+00:00","updated_at":"2026-07-05T11:12:54.167148+00:00"}