{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:MNWSKHTLQXDMQU5HJDQNIRU47P","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"c561f0f275040eafc19d61d839a5d00554f41da222e724d8a820246555961a88","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-11-01T06:52:23Z","title_canon_sha256":"881685d281b6345f1442cf76c6ae62cad909e32585cdb0ccd972dbd5659a658b"},"schema_version":"1.0","source":{"id":"1811.00259","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1811.00259","created_at":"2026-05-18T00:01:47Z"},{"alias_kind":"arxiv_version","alias_value":"1811.00259v1","created_at":"2026-05-18T00:01:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.00259","created_at":"2026-05-18T00:01:47Z"},{"alias_kind":"pith_short_12","alias_value":"MNWSKHTLQXDM","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_16","alias_value":"MNWSKHTLQXDMQU5H","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_8","alias_value":"MNWSKHTL","created_at":"2026-05-18T12:32:37Z"}],"graph_snapshots":[{"event_id":"sha256:00a826d28325dad2cdf94768620257ff50a01a42fb40a1a2ed58eab4a652fa34","target":"graph","created_at":"2026-05-18T00:01:47Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Semiconductive ZnO has shown to be a fascinating element for application in high-performance sensors. ZnO with various thicknesses (87-500 nm) was deposited on the surface of Co-based amorphous micro-wire (Co68.15Fe4.35Si12.5B15) using magnetron sputtering technique and the magnetoimpedance (MI) response was evaluated. The MI% increases monotonously up to the 240 nm thickness of the ZnO layer. By further increase in the ZnO layer thickness the MI% decreases. MI response and field sensitivity increased from 227% and 1.7 %/Oe for bare micro-wire up to 406% and 4.99 %/Oe for ZnO deposited micro-w","authors_text":"A. Dadsetan, M. Almasi Kashi, M. R. Hajiali, S.M. Mohseni","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-11-01T06:52:23Z","title":"Effect of sputter deposited ZnO thin layers on magnetoimpedance response and field sensitivity of Co-based micro-wires"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.00259","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:982687125eb3116d4ad7a9bc1e3d05acfbebc7b2a47cd9cc7fc229de9ee5d2e7","target":"record","created_at":"2026-05-18T00:01:47Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"c561f0f275040eafc19d61d839a5d00554f41da222e724d8a820246555961a88","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-11-01T06:52:23Z","title_canon_sha256":"881685d281b6345f1442cf76c6ae62cad909e32585cdb0ccd972dbd5659a658b"},"schema_version":"1.0","source":{"id":"1811.00259","kind":"arxiv","version":1}},"canonical_sha256":"636d251e6b85c6c853a748e0d4469cfbd366f7d01f5b39ca7d9e247c185e921a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"636d251e6b85c6c853a748e0d4469cfbd366f7d01f5b39ca7d9e247c185e921a","first_computed_at":"2026-05-18T00:01:47.682748Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:01:47.682748Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"A7x+ic6zfy480pS6t+flnsd3EzjgBDfCxo/FtcfzuWX2InHzyVvhoug/SvPt6wWhYsdWUZI90su7XsETtJocCA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:01:47.683564Z","signed_message":"canonical_sha256_bytes"},"source_id":"1811.00259","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:982687125eb3116d4ad7a9bc1e3d05acfbebc7b2a47cd9cc7fc229de9ee5d2e7","sha256:00a826d28325dad2cdf94768620257ff50a01a42fb40a1a2ed58eab4a652fa34"],"state_sha256":"ef821d255281ccfd17175f56bc3f6ede423bd7bc2d0f86534526b98f682b6601"}