{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:LJLZOK5D7VX7PQSGYS4IGIDFLD","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":"53e6a7fee7fcfd1cb90baef4ee1c07e3867f89cf7d2676c4d88b4a7908541605","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","nucl-th","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2009-05-25T06:28:00Z","title_canon_sha256":"50694ea40a72313525871ae2eb565584e445c57803a5f3da1f913a1216e461b4"},"schema_version":"1.0","source":{"id":"0905.3953","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0905.3953","created_at":"2026-05-18T02:19:34Z"},{"alias_kind":"arxiv_version","alias_value":"0905.3953v4","created_at":"2026-05-18T02:19:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0905.3953","created_at":"2026-05-18T02:19:34Z"},{"alias_kind":"pith_short_12","alias_value":"LJLZOK5D7VX7","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_16","alias_value":"LJLZOK5D7VX7PQSG","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_8","alias_value":"LJLZOK5D","created_at":"2026-05-18T12:26:00Z"}],"graph_snapshots":[{"event_id":"sha256:0c8480abb0754077fb0f82e9ab987de6604accf43b0d6b7c0ccea4e6874cc1da","target":"graph","created_at":"2026-05-18T02:19:34Z","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":"We explain the Fano peak (an asymmetric resonance peak) as an interference effect involving resonant states. We reveal that there are three types of Fano asymmetry according to their origins: the interference between a resonant state and an anti-resonant state, that between a resonant state and a bound state, and that between two resonant states. We show that the last two show the asymmetric energy dependence given by Fano, but the first one shows a slightly different form. In order to show the above, we analytically and microscopically derive a formula where we express the conductance purely ","authors_text":"Gonzalo Ordonez, Keita Sasada, Naomichi Hatano","cross_cats":["cond-mat.stat-mech","math-ph","math.MP","nucl-th","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2009-05-25T06:28:00Z","title":"Resonant Spectrum Analysis of the Conductance of Open Quantum System and Three Types of Fano Parameter"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0905.3953","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":"sha256:5988d9ef96dd2acf3617e4e3fef52656f9dd9d69b4d3debb71b5bc3b74ae9c38","target":"record","created_at":"2026-05-18T02:19:34Z","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":"53e6a7fee7fcfd1cb90baef4ee1c07e3867f89cf7d2676c4d88b4a7908541605","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","nucl-th","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2009-05-25T06:28:00Z","title_canon_sha256":"50694ea40a72313525871ae2eb565584e445c57803a5f3da1f913a1216e461b4"},"schema_version":"1.0","source":{"id":"0905.3953","kind":"arxiv","version":4}},"canonical_sha256":"5a57972ba3fd6ff7c246c4b883206558c7475f679d4047b9a4f2683adbe35f9c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5a57972ba3fd6ff7c246c4b883206558c7475f679d4047b9a4f2683adbe35f9c","first_computed_at":"2026-05-18T02:19:34.514563Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:19:34.514563Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8n3pXsdCQESJxodVgDmmL76T9ztK25j5VgrpHwb2UP21/wtsnb+ckVZIo1e1vQCZzPwHqYT3zl6tK1KvLwbgCw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:19:34.515121Z","signed_message":"canonical_sha256_bytes"},"source_id":"0905.3953","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5988d9ef96dd2acf3617e4e3fef52656f9dd9d69b4d3debb71b5bc3b74ae9c38","sha256:0c8480abb0754077fb0f82e9ab987de6604accf43b0d6b7c0ccea4e6874cc1da"],"state_sha256":"07ce82bc75669a26cf6f828476a3c4c11c72457809bad59dcf5db5dec17c9844"}