{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:A6ZSGPUGZ27M7UTLBUAO45EBR7","short_pith_number":"pith:A6ZSGPUG","canonical_record":{"source":{"id":"1407.1956","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-08T05:43:38Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"e9a2146b3418ea6141a0b465ebf178c9530467a755fab345af148f7b46eaa224","abstract_canon_sha256":"60ce5442ce4f102323c92d8fa3467742ee05ab303dae21cb8457349e52e5ef4e"},"schema_version":"1.0"},"canonical_sha256":"07b3233e86cebecfd26b0d00ee74818fe082cbaa53e0915ab7fd98dcb7379bdc","source":{"kind":"arxiv","id":"1407.1956","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.1956","created_at":"2026-05-18T02:47:22Z"},{"alias_kind":"arxiv_version","alias_value":"1407.1956v2","created_at":"2026-05-18T02:47:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.1956","created_at":"2026-05-18T02:47:22Z"},{"alias_kind":"pith_short_12","alias_value":"A6ZSGPUGZ27M","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_16","alias_value":"A6ZSGPUGZ27M7UTL","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_8","alias_value":"A6ZSGPUG","created_at":"2026-05-18T12:28:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:A6ZSGPUGZ27M7UTLBUAO45EBR7","target":"record","payload":{"canonical_record":{"source":{"id":"1407.1956","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-08T05:43:38Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"e9a2146b3418ea6141a0b465ebf178c9530467a755fab345af148f7b46eaa224","abstract_canon_sha256":"60ce5442ce4f102323c92d8fa3467742ee05ab303dae21cb8457349e52e5ef4e"},"schema_version":"1.0"},"canonical_sha256":"07b3233e86cebecfd26b0d00ee74818fe082cbaa53e0915ab7fd98dcb7379bdc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:47:22.710757Z","signature_b64":"4pzghNR9Q9+UA2/YGkrYpeWuCB2b8m/LlLn8PKMJElB2hFUM8NqZR2/fpvbxyBzRygRTBhG3oqtkPn2KoI8HAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07b3233e86cebecfd26b0d00ee74818fe082cbaa53e0915ab7fd98dcb7379bdc","last_reissued_at":"2026-05-18T02:47:22.710355Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:47:22.710355Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.1956","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:47:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"34i2o3rDzcybcPS+872nBJF2osBMgmALU0/DvHIUtT79w3T9EbYf9coC2+M26zCIptwuvbc38s0P68qZCap+Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T06:47:54.483454Z"},"content_sha256":"72daf458c58bfde895bbf8d6e481135d61ede6672381da5b6b86d25199a832a3","schema_version":"1.0","event_id":"sha256:72daf458c58bfde895bbf8d6e481135d61ede6672381da5b6b86d25199a832a3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:A6ZSGPUGZ27M7UTLBUAO45EBR7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Disorder-induced mutation of quasi-normal modes in 1D open systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.dis-nn","authors_text":"Franco Nori, Valentin Freilikher, Yury Bliokh","submitted_at":"2014-07-08T05:43:38Z","abstract_excerpt":"We study the relation between quasi-normal modes (QNMs) and transmission resonances (TRs) in one-dimensional (1D) disordered systems. We show for the first time that while each maximum in the transmission coefficient is always related to a QNM, the reverse statement is not necessarily correct. There exists an intermediate state, at which only a part of the QNMs are localized and these QNMs provide a resonant transmission. The rest of the solutions of the eigenvalue problem (denoted as strange quasi-modes) are never found in regular open cavities and resonators, and arise exclusively due to ran"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.1956","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:47:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vzfS9vJg6UOHaUzxX6k9tdn2KvuhEjej0j2OheYUgZiC7IgqKy/ptNWl5+sqgEJX2LbIolvCFicyNg233XT9CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T06:47:54.484064Z"},"content_sha256":"bca5d094ed7c379b150b44d1920e692b0f8b56b850fe797153b9c7ff619adf0b","schema_version":"1.0","event_id":"sha256:bca5d094ed7c379b150b44d1920e692b0f8b56b850fe797153b9c7ff619adf0b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/A6ZSGPUGZ27M7UTLBUAO45EBR7/bundle.json","state_url":"https://pith.science/pith/A6ZSGPUGZ27M7UTLBUAO45EBR7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/A6ZSGPUGZ27M7UTLBUAO45EBR7/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-01T06:47:54Z","links":{"resolver":"https://pith.science/pith/A6ZSGPUGZ27M7UTLBUAO45EBR7","bundle":"https://pith.science/pith/A6ZSGPUGZ27M7UTLBUAO45EBR7/bundle.json","state":"https://pith.science/pith/A6ZSGPUGZ27M7UTLBUAO45EBR7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/A6ZSGPUGZ27M7UTLBUAO45EBR7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:A6ZSGPUGZ27M7UTLBUAO45EBR7","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":"60ce5442ce4f102323c92d8fa3467742ee05ab303dae21cb8457349e52e5ef4e","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-08T05:43:38Z","title_canon_sha256":"e9a2146b3418ea6141a0b465ebf178c9530467a755fab345af148f7b46eaa224"},"schema_version":"1.0","source":{"id":"1407.1956","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.1956","created_at":"2026-05-18T02:47:22Z"},{"alias_kind":"arxiv_version","alias_value":"1407.1956v2","created_at":"2026-05-18T02:47:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.1956","created_at":"2026-05-18T02:47:22Z"},{"alias_kind":"pith_short_12","alias_value":"A6ZSGPUGZ27M","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_16","alias_value":"A6ZSGPUGZ27M7UTL","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_8","alias_value":"A6ZSGPUG","created_at":"2026-05-18T12:28:19Z"}],"graph_snapshots":[{"event_id":"sha256:bca5d094ed7c379b150b44d1920e692b0f8b56b850fe797153b9c7ff619adf0b","target":"graph","created_at":"2026-05-18T02:47:22Z","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":"We study the relation between quasi-normal modes (QNMs) and transmission resonances (TRs) in one-dimensional (1D) disordered systems. We show for the first time that while each maximum in the transmission coefficient is always related to a QNM, the reverse statement is not necessarily correct. There exists an intermediate state, at which only a part of the QNMs are localized and these QNMs provide a resonant transmission. The rest of the solutions of the eigenvalue problem (denoted as strange quasi-modes) are never found in regular open cavities and resonators, and arise exclusively due to ran","authors_text":"Franco Nori, Valentin Freilikher, Yury Bliokh","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-08T05:43:38Z","title":"Disorder-induced mutation of quasi-normal modes in 1D open systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.1956","kind":"arxiv","version":2},"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":"sha256:72daf458c58bfde895bbf8d6e481135d61ede6672381da5b6b86d25199a832a3","target":"record","created_at":"2026-05-18T02:47:22Z","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":"60ce5442ce4f102323c92d8fa3467742ee05ab303dae21cb8457349e52e5ef4e","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-08T05:43:38Z","title_canon_sha256":"e9a2146b3418ea6141a0b465ebf178c9530467a755fab345af148f7b46eaa224"},"schema_version":"1.0","source":{"id":"1407.1956","kind":"arxiv","version":2}},"canonical_sha256":"07b3233e86cebecfd26b0d00ee74818fe082cbaa53e0915ab7fd98dcb7379bdc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"07b3233e86cebecfd26b0d00ee74818fe082cbaa53e0915ab7fd98dcb7379bdc","first_computed_at":"2026-05-18T02:47:22.710355Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:47:22.710355Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4pzghNR9Q9+UA2/YGkrYpeWuCB2b8m/LlLn8PKMJElB2hFUM8NqZR2/fpvbxyBzRygRTBhG3oqtkPn2KoI8HAw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:47:22.710757Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.1956","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:72daf458c58bfde895bbf8d6e481135d61ede6672381da5b6b86d25199a832a3","sha256:bca5d094ed7c379b150b44d1920e692b0f8b56b850fe797153b9c7ff619adf0b"],"state_sha256":"7ecca1bed18437beaf00ea18b4a23906d694d17770727d5055d6a9a7e76667d4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nHxBu/Ze8hi3U3Hv3AbqjGJFs+XGqnj2qZndX1g2NSrgsFsTZ4dEiRQQiH+jEDe0PVbYjycHF1QWIuOI6VMOBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T06:47:54.487736Z","bundle_sha256":"6f46d37c5a8d473eef725beaa907b434684ab075b34e874e34612209cc863fb6"}}