{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:APIGK3MQ55ZUIB2AAQAO7CZC23","short_pith_number":"pith:APIGK3MQ","canonical_record":{"source":{"id":"cond-mat/0109346","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"2001-09-19T15:22:14Z","cross_cats_sorted":[],"title_canon_sha256":"6651e8de4a976733064c40c42f3b2d871f300319d265723a8001021550d25b48","abstract_canon_sha256":"8c03bfbc4c4fbb2f78a388977c4657f52cbab4f537c6f33454d8d6dc207377ee"},"schema_version":"1.0"},"canonical_sha256":"03d0656d90ef734407400400ef8b22d6dcd40c22e470962ddfeb1c13061789f7","source":{"kind":"arxiv","id":"cond-mat/0109346","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0109346","created_at":"2026-05-18T01:40:06Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0109346v3","created_at":"2026-05-18T01:40:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0109346","created_at":"2026-05-18T01:40:06Z"},{"alias_kind":"pith_short_12","alias_value":"APIGK3MQ55ZU","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"APIGK3MQ55ZUIB2A","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"APIGK3MQ","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:APIGK3MQ55ZUIB2AAQAO7CZC23","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0109346","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"2001-09-19T15:22:14Z","cross_cats_sorted":[],"title_canon_sha256":"6651e8de4a976733064c40c42f3b2d871f300319d265723a8001021550d25b48","abstract_canon_sha256":"8c03bfbc4c4fbb2f78a388977c4657f52cbab4f537c6f33454d8d6dc207377ee"},"schema_version":"1.0"},"canonical_sha256":"03d0656d90ef734407400400ef8b22d6dcd40c22e470962ddfeb1c13061789f7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:40:06.683325Z","signature_b64":"tywzM87Ec3NmJZTUut21ESKg+pQjVYDhtzGgffKLV4wPxylK47jWmndco9ewef1+KrPDJhdRAVhNnJ5VkkmRCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03d0656d90ef734407400400ef8b22d6dcd40c22e470962ddfeb1c13061789f7","last_reissued_at":"2026-05-18T01:40:06.682861Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:40:06.682861Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0109346","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:40:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7C2iqGG7mHxfJZuyiMDLWHS1hyDM6nqfzilSIqNI35t5DeFQDU7Dpn4o5DU4CyO1pqApepKJIxco79QDr1B1CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:28:07.879587Z"},"content_sha256":"03e0118ab7485e4485b7b57dd1ed9188f2e7ce6a2bc60a794e12a63a19548f6d","schema_version":"1.0","event_id":"sha256:03e0118ab7485e4485b7b57dd1ed9188f2e7ce6a2bc60a794e12a63a19548f6d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:APIGK3MQ55ZUIB2AAQAO7CZC23","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Large Deviation of the Density Profile in the Steady State of the Open Symmetric Simple Exclusion Process","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"B. Derrida, E. R. Speer, J. L. Lebowitz","submitted_at":"2001-09-19T15:22:14Z","abstract_excerpt":"We consider an open one dimensional lattice gas on sites $i=1,...,N$, with particles jumping independently with rate 1 to neighboring interior empty sites, the {\\it simple symmetric exclusion process}. The particle fluxes at the left and right boundaries, corresponding to exchanges with reservoirs at different chemical potentials, create a stationary nonequilibrium state (SNS) with a steady flux of particles through the system. The mean density profile in this state, which is linear, describes the typical behavior of a macroscopic system, i.e., this profile occurs with probability 1 when $N \\t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0109346","kind":"arxiv","version":3},"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":"2026-05-18T01:40:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jJ2790t2c1CKMIMFZwKjEinsatsVmrl/QQage1oZmxkn4UUoAcQYnYtGaTgRo2zby51UYgCnytGS3MZh9N2sAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:28:07.879965Z"},"content_sha256":"918378741b757e5509c2694d6d5fa32a9c46c5384f49a98c1338e68d31534a72","schema_version":"1.0","event_id":"sha256:918378741b757e5509c2694d6d5fa32a9c46c5384f49a98c1338e68d31534a72"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/APIGK3MQ55ZUIB2AAQAO7CZC23/bundle.json","state_url":"https://pith.science/pith/APIGK3MQ55ZUIB2AAQAO7CZC23/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/APIGK3MQ55ZUIB2AAQAO7CZC23/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":"2026-05-30T06:28:07Z","links":{"resolver":"https://pith.science/pith/APIGK3MQ55ZUIB2AAQAO7CZC23","bundle":"https://pith.science/pith/APIGK3MQ55ZUIB2AAQAO7CZC23/bundle.json","state":"https://pith.science/pith/APIGK3MQ55ZUIB2AAQAO7CZC23/state.json","well_known_bundle":"https://pith.science/.well-known/pith/APIGK3MQ55ZUIB2AAQAO7CZC23/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:APIGK3MQ55ZUIB2AAQAO7CZC23","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":"8c03bfbc4c4fbb2f78a388977c4657f52cbab4f537c6f33454d8d6dc207377ee","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat","submitted_at":"2001-09-19T15:22:14Z","title_canon_sha256":"6651e8de4a976733064c40c42f3b2d871f300319d265723a8001021550d25b48"},"schema_version":"1.0","source":{"id":"cond-mat/0109346","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0109346","created_at":"2026-05-18T01:40:06Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0109346v3","created_at":"2026-05-18T01:40:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0109346","created_at":"2026-05-18T01:40:06Z"},{"alias_kind":"pith_short_12","alias_value":"APIGK3MQ55ZU","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"APIGK3MQ55ZUIB2A","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"APIGK3MQ","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:918378741b757e5509c2694d6d5fa32a9c46c5384f49a98c1338e68d31534a72","target":"graph","created_at":"2026-05-18T01:40:06Z","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 consider an open one dimensional lattice gas on sites $i=1,...,N$, with particles jumping independently with rate 1 to neighboring interior empty sites, the {\\it simple symmetric exclusion process}. The particle fluxes at the left and right boundaries, corresponding to exchanges with reservoirs at different chemical potentials, create a stationary nonequilibrium state (SNS) with a steady flux of particles through the system. The mean density profile in this state, which is linear, describes the typical behavior of a macroscopic system, i.e., this profile occurs with probability 1 when $N \\t","authors_text":"B. Derrida, E. R. Speer, J. L. Lebowitz","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat","submitted_at":"2001-09-19T15:22:14Z","title":"Large Deviation of the Density Profile in the Steady State of the Open Symmetric Simple Exclusion Process"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0109346","kind":"arxiv","version":3},"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":"sha256:03e0118ab7485e4485b7b57dd1ed9188f2e7ce6a2bc60a794e12a63a19548f6d","target":"record","created_at":"2026-05-18T01:40:06Z","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":"8c03bfbc4c4fbb2f78a388977c4657f52cbab4f537c6f33454d8d6dc207377ee","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat","submitted_at":"2001-09-19T15:22:14Z","title_canon_sha256":"6651e8de4a976733064c40c42f3b2d871f300319d265723a8001021550d25b48"},"schema_version":"1.0","source":{"id":"cond-mat/0109346","kind":"arxiv","version":3}},"canonical_sha256":"03d0656d90ef734407400400ef8b22d6dcd40c22e470962ddfeb1c13061789f7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"03d0656d90ef734407400400ef8b22d6dcd40c22e470962ddfeb1c13061789f7","first_computed_at":"2026-05-18T01:40:06.682861Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:40:06.682861Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tywzM87Ec3NmJZTUut21ESKg+pQjVYDhtzGgffKLV4wPxylK47jWmndco9ewef1+KrPDJhdRAVhNnJ5VkkmRCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:40:06.683325Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0109346","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:03e0118ab7485e4485b7b57dd1ed9188f2e7ce6a2bc60a794e12a63a19548f6d","sha256:918378741b757e5509c2694d6d5fa32a9c46c5384f49a98c1338e68d31534a72"],"state_sha256":"0142c24e2f36a319e81d6728d2a73ef4a1ebcae52dc2db23ae7254925c546a85"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HJL+z5bNeNFVKbg2rsg4NVdQGn/sPgJJ05oBtlT08224Rr+gw5CU7a/NKkVyMmOjxb/wCuG3zh/MBtLs89BWDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T06:28:07.883279Z","bundle_sha256":"9605a41f9585146a2b79c704a032047243f4788ed4a1e3fbf5af53c1c780e436"}}