{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:67QN3JPOALI4Z7STVCD7CZSPJU","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":"6392252eabdf1fa1579df5ce6c1d5e57bffe2977582fd5690c1682cd8d115f06","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-02-10T08:55:43Z","title_canon_sha256":"134713883a4edcfcbc9f66986cee4b51688a543b0eaaf685d09a55855a370efd"},"schema_version":"1.0","source":{"id":"1702.03103","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.03103","created_at":"2026-05-17T23:58:50Z"},{"alias_kind":"arxiv_version","alias_value":"1702.03103v1","created_at":"2026-05-17T23:58:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.03103","created_at":"2026-05-17T23:58:50Z"},{"alias_kind":"pith_short_12","alias_value":"67QN3JPOALI4","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"67QN3JPOALI4Z7ST","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"67QN3JPO","created_at":"2026-05-18T12:31:03Z"}],"graph_snapshots":[{"event_id":"sha256:fc144bce8457a88e74b309986ff241d774d44aebd8bf3671dfb40195f4d462c0","target":"graph","created_at":"2026-05-17T23:58:50Z","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":"Exact quantitative understanding of plasmon propagation along nanowires is mandatory for designing and creating functional devices. Here we investigate plasmon transmission through top-down fabricated monocrystalline gold nanowires on a glass substrate. We show that the transmission through finite-length nanowires can be described by Fabry-P\\'{e}rot oscillations that beat with free-space propagating light launched at the incoupling end. Using an extended Fabry-P\\'{e}rot model, experimental and simulated length dependent transmission signals agree quantitatively with a fully analytical model.","authors_text":"Bert Hecht, Enno Krauss, Gary Razinskas, Peter Geisler","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-02-10T08:55:43Z","title":"Transmission of plasmons through a nanowire"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.03103","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":"sha256:514330becf89f556904f2cfafb74c20278657cc9ce85adee7f4286f1b67fd341","target":"record","created_at":"2026-05-17T23:58:50Z","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":"6392252eabdf1fa1579df5ce6c1d5e57bffe2977582fd5690c1682cd8d115f06","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-02-10T08:55:43Z","title_canon_sha256":"134713883a4edcfcbc9f66986cee4b51688a543b0eaaf685d09a55855a370efd"},"schema_version":"1.0","source":{"id":"1702.03103","kind":"arxiv","version":1}},"canonical_sha256":"f7e0dda5ee02d1ccfe53a887f1664f4d09ffc42323bc4f42c916abcd31ceba52","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f7e0dda5ee02d1ccfe53a887f1664f4d09ffc42323bc4f42c916abcd31ceba52","first_computed_at":"2026-05-17T23:58:50.353530Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:58:50.353530Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NlsUTdh9jtGcecLYfTTDcdjiqVLUaFzuLJ++Nf3C2RwGdL8s+qr/NyXOrdl2gKnmSyzAz+AGSv2itNUgAlwdDg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:58:50.353984Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.03103","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:514330becf89f556904f2cfafb74c20278657cc9ce85adee7f4286f1b67fd341","sha256:fc144bce8457a88e74b309986ff241d774d44aebd8bf3671dfb40195f4d462c0"],"state_sha256":"cb965f2fa962c4c7976cd085d0c8c44dbbb0f2dff35ddb2295cc18d31238c497"}