{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:GSOZBARAWX4JX5MHHSKBIZEN6Z","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":"74ed6f14ed4cadf32c6c4972b24f1a55f27b2659e742eb5cd7fd494385a538fa","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el","cond-mat.supr-con","math-ph","math.MP","nlin.SI","physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-02-17T22:17:27Z","title_canon_sha256":"fa8216769944609c1ba195e9b4b4cb4ddd62d164c581e8dd89990672e8bc02d8"},"schema_version":"1.0","source":{"id":"0902.3014","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0902.3014","created_at":"2026-05-18T04:42:22Z"},{"alias_kind":"arxiv_version","alias_value":"0902.3014v4","created_at":"2026-05-18T04:42:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0902.3014","created_at":"2026-05-18T04:42:22Z"},{"alias_kind":"pith_short_12","alias_value":"GSOZBARAWX4J","created_at":"2026-05-18T12:25:59Z"},{"alias_kind":"pith_short_16","alias_value":"GSOZBARAWX4JX5MH","created_at":"2026-05-18T12:25:59Z"},{"alias_kind":"pith_short_8","alias_value":"GSOZBARA","created_at":"2026-05-18T12:25:59Z"}],"graph_snapshots":[{"event_id":"sha256:87ce2c9459231bfebc79b067e37bfafd4f6227fd746494fa8657c38ed76f0f05","target":"graph","created_at":"2026-05-18T04:42:22Z","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":"Nowadays nanotechnology allows to scale-down various important devices (sensors, chips, fibres, etc), and, thus, opens up new horizon for their applications. Nevertheless, the efficiency most of them is still based on the fundamental physical phenomena, such as resonances. Thus, the understanding of the resonance phenomena will be beneficial. One of the well-known examples is the resonant enhancement of the transmission known as Breit-Wigner resonances, which can be described by a Lorentzian function. But, in many physical systems the scattering of waves involves propagation along different pa","authors_text":"Andrey E. Miroshnichenko, Sergej Flach, Yuri S. Kivshar","cross_cats":["cond-mat.mes-hall","cond-mat.str-el","cond-mat.supr-con","math-ph","math.MP","nlin.SI","physics.atom-ph","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-02-17T22:17:27Z","title":"Fano resonances in nanoscale structures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0902.3014","kind":"arxiv","version":4},"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":"sha256:555d3102606c927577c1f9fe32b938d12bceab602a67b36c69ed58a7c19bc44f","target":"record","created_at":"2026-05-18T04:42:22Z","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":"74ed6f14ed4cadf32c6c4972b24f1a55f27b2659e742eb5cd7fd494385a538fa","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el","cond-mat.supr-con","math-ph","math.MP","nlin.SI","physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2009-02-17T22:17:27Z","title_canon_sha256":"fa8216769944609c1ba195e9b4b4cb4ddd62d164c581e8dd89990672e8bc02d8"},"schema_version":"1.0","source":{"id":"0902.3014","kind":"arxiv","version":4}},"canonical_sha256":"349d908220b5f89bf5873c9414648df642587ff1a7f78d2bc0bb89fc19fbf52a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"349d908220b5f89bf5873c9414648df642587ff1a7f78d2bc0bb89fc19fbf52a","first_computed_at":"2026-05-18T04:42:22.191456Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:42:22.191456Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0cnlcd4GPhlmvzksXS9ppZPHdwJ7k5uH6mGylnyWWhsSJLLy4kbjILCgvH21at/1uku33Ei1pOIKe94H+dYeBg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:42:22.191956Z","signed_message":"canonical_sha256_bytes"},"source_id":"0902.3014","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:555d3102606c927577c1f9fe32b938d12bceab602a67b36c69ed58a7c19bc44f","sha256:87ce2c9459231bfebc79b067e37bfafd4f6227fd746494fa8657c38ed76f0f05"],"state_sha256":"6445ca4a0ae6ac018b67f2bf61438e0e20a5798d233f95eed80df3f08bb7e4b7"}