{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:TCJD37Q6TIO67OMDTP2P4MSJSE","short_pith_number":"pith:TCJD37Q6","canonical_record":{"source":{"id":"1505.02116","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-05-08T18:15:13Z","cross_cats_sorted":[],"title_canon_sha256":"7eb76713040acff68e109f7703d5728332738f55f1d6be9ae7b2ded6b3817238","abstract_canon_sha256":"50e62c086946ce47cc04d797786195938283a5a6af5befd05f00af4bb9941220"},"schema_version":"1.0"},"canonical_sha256":"98923dfe1e9a1defb9839bf4fe3249911e1b7d83518869bdfb780a938b7e8f9c","source":{"kind":"arxiv","id":"1505.02116","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.02116","created_at":"2026-05-18T01:22:40Z"},{"alias_kind":"arxiv_version","alias_value":"1505.02116v1","created_at":"2026-05-18T01:22:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.02116","created_at":"2026-05-18T01:22:40Z"},{"alias_kind":"pith_short_12","alias_value":"TCJD37Q6TIO6","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_16","alias_value":"TCJD37Q6TIO67OMD","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_8","alias_value":"TCJD37Q6","created_at":"2026-05-18T12:29:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:TCJD37Q6TIO67OMDTP2P4MSJSE","target":"record","payload":{"canonical_record":{"source":{"id":"1505.02116","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-05-08T18:15:13Z","cross_cats_sorted":[],"title_canon_sha256":"7eb76713040acff68e109f7703d5728332738f55f1d6be9ae7b2ded6b3817238","abstract_canon_sha256":"50e62c086946ce47cc04d797786195938283a5a6af5befd05f00af4bb9941220"},"schema_version":"1.0"},"canonical_sha256":"98923dfe1e9a1defb9839bf4fe3249911e1b7d83518869bdfb780a938b7e8f9c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:40.272247Z","signature_b64":"Wl7u3pFUv6ir2SpHPnY88Xdldse+UnyzZiIh1Psra9V0mSMeSrqYHd9Z90XCi+n8v50qYQiqgj++2oMNhiurAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"98923dfe1e9a1defb9839bf4fe3249911e1b7d83518869bdfb780a938b7e8f9c","last_reissued_at":"2026-05-18T01:22:40.271676Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:40.271676Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1505.02116","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:22:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PKvmOFiNkPPUIaJIkWFX3EA/8WPPGLe+RJYoA5NkaE88RWX1FizBg0kqpTx6IJEe3A8m0s4E9RKit4vD4uiQCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:59:32.140283Z"},"content_sha256":"e6b5e015188a6f1ecd2f98aad7642b7fc4986c2a7330a53d2032f6f4163ede83","schema_version":"1.0","event_id":"sha256:e6b5e015188a6f1ecd2f98aad7642b7fc4986c2a7330a53d2032f6f4163ede83"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:TCJD37Q6TIO67OMDTP2P4MSJSE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Perturbative fluctuation dissipation relation for non-equilibrium finite frequency noise in quantum circuits","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Benjamin Roussel, In\\`es Safi, Pascal Degiovanni","submitted_at":"2015-05-08T18:15:13Z","abstract_excerpt":"We develop a general perturbative computation of finite-frequency quantum noise which applies, in particular, to both good or weakly transmitting strongly correlated conductors coupled to a generic environment. Under a minimal set of hypotheses, we show that the noise can be expressed through the non-equilibrium DC current only, generalizing a non-equilibrium fluctuation dissipation relation. We use this relation to derive explicit predictions for the non equilibrium finite frequency noise for a single channel conductor connected to an arbitrary Ohmic environment."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.02116","kind":"arxiv","version":1},"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":"2026-05-18T01:22:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DpzOPrAVjZm+Sx3Mgx6AoM52jmCzpnxH30EhDF61AWzJVS40Q77TTt+AU4eESfKzp4bBeWjt6PZRzq/IG2JbCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:59:32.140653Z"},"content_sha256":"a1bf57351ce72f45df260df39a9d499de499744304877b89a2c94152ce769631","schema_version":"1.0","event_id":"sha256:a1bf57351ce72f45df260df39a9d499de499744304877b89a2c94152ce769631"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TCJD37Q6TIO67OMDTP2P4MSJSE/bundle.json","state_url":"https://pith.science/pith/TCJD37Q6TIO67OMDTP2P4MSJSE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TCJD37Q6TIO67OMDTP2P4MSJSE/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":"2026-06-01T00:59:32Z","links":{"resolver":"https://pith.science/pith/TCJD37Q6TIO67OMDTP2P4MSJSE","bundle":"https://pith.science/pith/TCJD37Q6TIO67OMDTP2P4MSJSE/bundle.json","state":"https://pith.science/pith/TCJD37Q6TIO67OMDTP2P4MSJSE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TCJD37Q6TIO67OMDTP2P4MSJSE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:TCJD37Q6TIO67OMDTP2P4MSJSE","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":"50e62c086946ce47cc04d797786195938283a5a6af5befd05f00af4bb9941220","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-05-08T18:15:13Z","title_canon_sha256":"7eb76713040acff68e109f7703d5728332738f55f1d6be9ae7b2ded6b3817238"},"schema_version":"1.0","source":{"id":"1505.02116","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.02116","created_at":"2026-05-18T01:22:40Z"},{"alias_kind":"arxiv_version","alias_value":"1505.02116v1","created_at":"2026-05-18T01:22:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.02116","created_at":"2026-05-18T01:22:40Z"},{"alias_kind":"pith_short_12","alias_value":"TCJD37Q6TIO6","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_16","alias_value":"TCJD37Q6TIO67OMD","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_8","alias_value":"TCJD37Q6","created_at":"2026-05-18T12:29:42Z"}],"graph_snapshots":[{"event_id":"sha256:a1bf57351ce72f45df260df39a9d499de499744304877b89a2c94152ce769631","target":"graph","created_at":"2026-05-18T01:22:40Z","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 develop a general perturbative computation of finite-frequency quantum noise which applies, in particular, to both good or weakly transmitting strongly correlated conductors coupled to a generic environment. Under a minimal set of hypotheses, we show that the noise can be expressed through the non-equilibrium DC current only, generalizing a non-equilibrium fluctuation dissipation relation. We use this relation to derive explicit predictions for the non equilibrium finite frequency noise for a single channel conductor connected to an arbitrary Ohmic environment.","authors_text":"Benjamin Roussel, In\\`es Safi, Pascal Degiovanni","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-05-08T18:15:13Z","title":"Perturbative fluctuation dissipation relation for non-equilibrium finite frequency noise in quantum circuits"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.02116","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:e6b5e015188a6f1ecd2f98aad7642b7fc4986c2a7330a53d2032f6f4163ede83","target":"record","created_at":"2026-05-18T01:22:40Z","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":"50e62c086946ce47cc04d797786195938283a5a6af5befd05f00af4bb9941220","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-05-08T18:15:13Z","title_canon_sha256":"7eb76713040acff68e109f7703d5728332738f55f1d6be9ae7b2ded6b3817238"},"schema_version":"1.0","source":{"id":"1505.02116","kind":"arxiv","version":1}},"canonical_sha256":"98923dfe1e9a1defb9839bf4fe3249911e1b7d83518869bdfb780a938b7e8f9c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"98923dfe1e9a1defb9839bf4fe3249911e1b7d83518869bdfb780a938b7e8f9c","first_computed_at":"2026-05-18T01:22:40.271676Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:22:40.271676Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Wl7u3pFUv6ir2SpHPnY88Xdldse+UnyzZiIh1Psra9V0mSMeSrqYHd9Z90XCi+n8v50qYQiqgj++2oMNhiurAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:22:40.272247Z","signed_message":"canonical_sha256_bytes"},"source_id":"1505.02116","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e6b5e015188a6f1ecd2f98aad7642b7fc4986c2a7330a53d2032f6f4163ede83","sha256:a1bf57351ce72f45df260df39a9d499de499744304877b89a2c94152ce769631"],"state_sha256":"5c501405649ca97b2447d69b31b236329460b4ce5415f6b677b640d0a93c2395"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZWs9FStZ0mLaBgTwAtrWDdlDTiQ07g6eTSy3hd15PN3gfT1QCOhOzN2VV9PWpt6kDquKhZ1g2pQ/9HzsDNw1Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T00:59:32.142996Z","bundle_sha256":"f58171a2f0137585de57398da430896853cdd0c37d37a4b8c766c5f79a5db666"}}