{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:3WTIYS4W4WNNECUPEJ2IMDB3GG","short_pith_number":"pith:3WTIYS4W","canonical_record":{"source":{"id":"1306.5135","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-06-21T13:27:57Z","cross_cats_sorted":[],"title_canon_sha256":"0fef38324ed012a1e4ba2054a6954bffe6bff45848a33dec6f31270de81725b0","abstract_canon_sha256":"285046d700ea87020b1a2241d4621008df6cb08548668a11b2ed7acebdb63770"},"schema_version":"1.0"},"canonical_sha256":"dda68c4b96e59ad20a8f2274860c3b318eaf835867296a9316760f667459bd73","source":{"kind":"arxiv","id":"1306.5135","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.5135","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"arxiv_version","alias_value":"1306.5135v2","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.5135","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"pith_short_12","alias_value":"3WTIYS4W4WNN","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_16","alias_value":"3WTIYS4W4WNNECUP","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_8","alias_value":"3WTIYS4W","created_at":"2026-05-18T12:27:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:3WTIYS4W4WNNECUPEJ2IMDB3GG","target":"record","payload":{"canonical_record":{"source":{"id":"1306.5135","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-06-21T13:27:57Z","cross_cats_sorted":[],"title_canon_sha256":"0fef38324ed012a1e4ba2054a6954bffe6bff45848a33dec6f31270de81725b0","abstract_canon_sha256":"285046d700ea87020b1a2241d4621008df6cb08548668a11b2ed7acebdb63770"},"schema_version":"1.0"},"canonical_sha256":"dda68c4b96e59ad20a8f2274860c3b318eaf835867296a9316760f667459bd73","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:06:21.988883Z","signature_b64":"ymVzauRUUidxRLFuuK/pSr9t7B5RYCu151SsXzmypGrmYJ7RjoaYh3Zf/ezIH2Cd0isDs76zwJ2ab+yTr0pMCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dda68c4b96e59ad20a8f2274860c3b318eaf835867296a9316760f667459bd73","last_reissued_at":"2026-05-18T03:06:21.988481Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:06:21.988481Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1306.5135","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":"2026-05-18T03:06:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PNgUjcIjRnXV6iULfSnA6pRbkxFlhFlsH/V9VN5BVQmYu+vpwkzXcwsNALQV0YRV3fX8Ubb5Pw54ZKvAACaqAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T01:14:13.092854Z"},"content_sha256":"b985f7b0018d6608f4bcb60f1dadd1714249bdf02098d8a573d559570069e85f","schema_version":"1.0","event_id":"sha256:b985f7b0018d6608f4bcb60f1dadd1714249bdf02098d8a573d559570069e85f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:3WTIYS4W4WNNECUPEJ2IMDB3GG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical Coulomb Blockade in an interacting 1D system coupled to an arbitrary environment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"I. Safi, J.-R. Souquet, P. Simon","submitted_at":"2013-06-21T13:27:57Z","abstract_excerpt":"We study the out-of-equilibrium transport in a Tomonaga-Luttinger liquid containing a weak or a tunneling barrier coupled to an arbitrary electromagnetic environment. This applies as well to a coherent one-channel non-interacting conductor with a transmission coefficient close to one or to zero. We derive formal expressions for the current and finite-frequency (FF) noise at arbitrary voltages, temperatures and frequency-dependent impedance $Z(\\omega)$ in the regimes of weak and strong backscattering. We show that these two regimes are no longer related by duality at finite frequency. We then c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.5135","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":"2026-05-18T03:06:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QZXwwZypZfXVNMzayryslzf5OH7s93ROt6QQJlcowLG+2r9pxohDT/ON7Uqe+LET1/825ELaIbJDRdMQ3HzuBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T01:14:13.093210Z"},"content_sha256":"d19e92215da8446500ddd3a880583988cde1aa87966a7c840e59aed926d09229","schema_version":"1.0","event_id":"sha256:d19e92215da8446500ddd3a880583988cde1aa87966a7c840e59aed926d09229"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3WTIYS4W4WNNECUPEJ2IMDB3GG/bundle.json","state_url":"https://pith.science/pith/3WTIYS4W4WNNECUPEJ2IMDB3GG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3WTIYS4W4WNNECUPEJ2IMDB3GG/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":"2026-06-03T01:14:13Z","links":{"resolver":"https://pith.science/pith/3WTIYS4W4WNNECUPEJ2IMDB3GG","bundle":"https://pith.science/pith/3WTIYS4W4WNNECUPEJ2IMDB3GG/bundle.json","state":"https://pith.science/pith/3WTIYS4W4WNNECUPEJ2IMDB3GG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3WTIYS4W4WNNECUPEJ2IMDB3GG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:3WTIYS4W4WNNECUPEJ2IMDB3GG","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":"285046d700ea87020b1a2241d4621008df6cb08548668a11b2ed7acebdb63770","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-06-21T13:27:57Z","title_canon_sha256":"0fef38324ed012a1e4ba2054a6954bffe6bff45848a33dec6f31270de81725b0"},"schema_version":"1.0","source":{"id":"1306.5135","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.5135","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"arxiv_version","alias_value":"1306.5135v2","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.5135","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"pith_short_12","alias_value":"3WTIYS4W4WNN","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_16","alias_value":"3WTIYS4W4WNNECUP","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_8","alias_value":"3WTIYS4W","created_at":"2026-05-18T12:27:32Z"}],"graph_snapshots":[{"event_id":"sha256:d19e92215da8446500ddd3a880583988cde1aa87966a7c840e59aed926d09229","target":"graph","created_at":"2026-05-18T03:06:21Z","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 out-of-equilibrium transport in a Tomonaga-Luttinger liquid containing a weak or a tunneling barrier coupled to an arbitrary electromagnetic environment. This applies as well to a coherent one-channel non-interacting conductor with a transmission coefficient close to one or to zero. We derive formal expressions for the current and finite-frequency (FF) noise at arbitrary voltages, temperatures and frequency-dependent impedance $Z(\\omega)$ in the regimes of weak and strong backscattering. We show that these two regimes are no longer related by duality at finite frequency. We then c","authors_text":"I. Safi, J.-R. Souquet, P. Simon","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-06-21T13:27:57Z","title":"Dynamical Coulomb Blockade in an interacting 1D system coupled to an arbitrary environment"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.5135","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:b985f7b0018d6608f4bcb60f1dadd1714249bdf02098d8a573d559570069e85f","target":"record","created_at":"2026-05-18T03:06:21Z","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":"285046d700ea87020b1a2241d4621008df6cb08548668a11b2ed7acebdb63770","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-06-21T13:27:57Z","title_canon_sha256":"0fef38324ed012a1e4ba2054a6954bffe6bff45848a33dec6f31270de81725b0"},"schema_version":"1.0","source":{"id":"1306.5135","kind":"arxiv","version":2}},"canonical_sha256":"dda68c4b96e59ad20a8f2274860c3b318eaf835867296a9316760f667459bd73","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dda68c4b96e59ad20a8f2274860c3b318eaf835867296a9316760f667459bd73","first_computed_at":"2026-05-18T03:06:21.988481Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:06:21.988481Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ymVzauRUUidxRLFuuK/pSr9t7B5RYCu151SsXzmypGrmYJ7RjoaYh3Zf/ezIH2Cd0isDs76zwJ2ab+yTr0pMCA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:06:21.988883Z","signed_message":"canonical_sha256_bytes"},"source_id":"1306.5135","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b985f7b0018d6608f4bcb60f1dadd1714249bdf02098d8a573d559570069e85f","sha256:d19e92215da8446500ddd3a880583988cde1aa87966a7c840e59aed926d09229"],"state_sha256":"e82c87937ba73dafd97d8631f6993dbc059f6120084deb2cce29e7844ceec4e4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wXbTKBwWmLkp6mbljbnE6lUU/G/4Frs4RtiD9Jti7apoPQc2cdLVfw6mJ1u8UhtX8PnguiM4LTgrVd0CRvKRDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T01:14:13.095122Z","bundle_sha256":"fb7cae4d133b8e12212d089b867a58426b08a5a245fca6df599b00f3f34e0b77"}}