{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:6HKBNX5S4ECHWY2FOJUHEA3BMS","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":"9b150d68422cf1a3957e870b21ffa2aa7f574d8dce7afe85aca08fb34a3b9255","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-06-08T14:10:49Z","title_canon_sha256":"8955563ac0d71bd46438a7ea3124e44e28acf643929535cd521d029778e060e0"},"schema_version":"1.0","source":{"id":"2606.09523","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.09523","created_at":"2026-06-09T02:08:53Z"},{"alias_kind":"arxiv_version","alias_value":"2606.09523v1","created_at":"2026-06-09T02:08:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.09523","created_at":"2026-06-09T02:08:53Z"},{"alias_kind":"pith_short_12","alias_value":"6HKBNX5S4ECH","created_at":"2026-06-09T02:08:53Z"},{"alias_kind":"pith_short_16","alias_value":"6HKBNX5S4ECHWY2F","created_at":"2026-06-09T02:08:53Z"},{"alias_kind":"pith_short_8","alias_value":"6HKBNX5S","created_at":"2026-06-09T02:08:53Z"}],"graph_snapshots":[{"event_id":"sha256:e0a1ca290f81f9cf904d7473efbd3c9b53f01bc0c6837a1455c339177aef9a60","target":"graph","created_at":"2026-06-09T02:08:53Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2606.09523/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We introduce a unified theoretical framework for single-plasmon transport in one-dimensional nanowires, bridging the quantized electromagnetic Green's tensor formalism with effective non-Hermitian Hamiltonian models. This approach naturally incorporates propagating surface plasmon polaritons, high-order modes dissipative channels, and intrinsic losses. We investigate both the stationary regime and the spatio-temporal dynamics of a single-plasmon pulse travelling through an atomic chain coupled to a dispersive nanowire. We analyze modal contributions to reflection and transmission spectra for q","authors_text":"A. A. D{\\i}az-Valles, A. Leray, B. Rousseaux, G. Colas des Francs, H. Jauslin, S. Gu\\'erin","cross_cats":["cond-mat.mes-hall","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-06-08T14:10:49Z","title":"Single plasmon transport in one dimensional nanowire"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.09523","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":"sha256:0471a8f36232b732ec6a31d6dc86d76297c411ca1c7bf6c5977e2a543f804d8b","target":"record","created_at":"2026-06-09T02:08:53Z","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":"9b150d68422cf1a3957e870b21ffa2aa7f574d8dce7afe85aca08fb34a3b9255","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-06-08T14:10:49Z","title_canon_sha256":"8955563ac0d71bd46438a7ea3124e44e28acf643929535cd521d029778e060e0"},"schema_version":"1.0","source":{"id":"2606.09523","kind":"arxiv","version":1}},"canonical_sha256":"f1d416dfb2e1047b6345726872036164a7f158b71923a6822896ef6111bbc138","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f1d416dfb2e1047b6345726872036164a7f158b71923a6822896ef6111bbc138","first_computed_at":"2026-06-09T02:08:53.265879Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-09T02:08:53.265879Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Fj66jN7h+iWvAKezsHxvg2UGoCn28pWrfTr/GTVRJ1dXyy58/kwhOpbWrLlfLNWybF/NWE0Q2EKr52obxIR4CA==","signature_status":"signed_v1","signed_at":"2026-06-09T02:08:53.266669Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.09523","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0471a8f36232b732ec6a31d6dc86d76297c411ca1c7bf6c5977e2a543f804d8b","sha256:e0a1ca290f81f9cf904d7473efbd3c9b53f01bc0c6837a1455c339177aef9a60"],"state_sha256":"22be2ef33cdc1c15dc3087f69ce5d11651aff888e80d958b37b9924ad31744c5"}