{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:OAYTSPINQD6HL6C5EYMECAYHIG","short_pith_number":"pith:OAYTSPIN","canonical_record":{"source":{"id":"1201.2749","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-01-13T07:17:54Z","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"title_canon_sha256":"880af7c969987665ba95549c3fa49610231d9dd0408e373b45b83d7bf69e64bf","abstract_canon_sha256":"82b6cc8819673c303dc4bced4e49e401c147a56c07e6fc892b6dedfabd9c5512"},"schema_version":"1.0"},"canonical_sha256":"7031393d0d80fc75f85d261841030741abdcf4156afa124bfe17c25a71e9f69d","source":{"kind":"arxiv","id":"1201.2749","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.2749","created_at":"2026-05-18T03:57:26Z"},{"alias_kind":"arxiv_version","alias_value":"1201.2749v3","created_at":"2026-05-18T03:57:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.2749","created_at":"2026-05-18T03:57:26Z"},{"alias_kind":"pith_short_12","alias_value":"OAYTSPINQD6H","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"OAYTSPINQD6HL6C5","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"OAYTSPIN","created_at":"2026-05-18T12:27:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:OAYTSPINQD6HL6C5EYMECAYHIG","target":"record","payload":{"canonical_record":{"source":{"id":"1201.2749","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-01-13T07:17:54Z","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"title_canon_sha256":"880af7c969987665ba95549c3fa49610231d9dd0408e373b45b83d7bf69e64bf","abstract_canon_sha256":"82b6cc8819673c303dc4bced4e49e401c147a56c07e6fc892b6dedfabd9c5512"},"schema_version":"1.0"},"canonical_sha256":"7031393d0d80fc75f85d261841030741abdcf4156afa124bfe17c25a71e9f69d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:57:26.622738Z","signature_b64":"u6gW35mJC6N85DyPcGXZuHRPEyTGnGdt+UGFFwa5y9k8/H7VmuwkLu9sy+t88tv8OA3DIJdSLIUbuesrVOLMDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7031393d0d80fc75f85d261841030741abdcf4156afa124bfe17c25a71e9f69d","last_reissued_at":"2026-05-18T03:57:26.621966Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:57:26.621966Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.2749","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":"2026-05-18T03:57:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OTeQ2j1TPXwyRzzlfY2cT90x5fUEd9QiuzCMu6a05tWbvR/YlCoW6wGUbJvhC98EWa3GpXsZbYWxLCHrZSTBAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T07:32:58.345090Z"},"content_sha256":"3c3e2684e8f10f65dba8dc847f096a04a8336003d590b8d50b294d2ede3c88cb","schema_version":"1.0","event_id":"sha256:3c3e2684e8f10f65dba8dc847f096a04a8336003d590b8d50b294d2ede3c88cb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:OAYTSPINQD6HL6C5EYMECAYHIG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Exact Relaxation Dynamics in the Totally Asymmetric Simple Exclusion Process","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","nlin.SI"],"primary_cat":"cond-mat.stat-mech","authors_text":"Jun Sato, Kazumitsu Sakai, Kohei Motegi","submitted_at":"2012-01-13T07:17:54Z","abstract_excerpt":"The relaxation dynamics of the one-dimensional totally asymmetric simple exclusion process on a ring is considered in the case of step initial condition. Analyzing the time evolution of the local particle densities and currents by the Bethe ansatz method, we examine their full relaxation dynamics. As a result, we observe peculiar behaviors, such as the emergence of a ripple in the density profile and the existence of the excessive particle currents. Moreover, by making a finite-size scaling analysis of the asymptotic amplitudes of the local densities and currents, we find the scaling exponents"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.2749","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":"2026-05-18T03:57:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nVjg43Iuap5Fs/PkGzwOnENwG1ocJ5rHH79Tn4GFED18R84A08xwYDVzHsF92jkaZ5Cq4ScsuXjzdVL7wlzRDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T07:32:58.345778Z"},"content_sha256":"9ba25d17f5e1631a6db358e8df6ce0437fa6d90e34ae731fa5d20aad6aa4d426","schema_version":"1.0","event_id":"sha256:9ba25d17f5e1631a6db358e8df6ce0437fa6d90e34ae731fa5d20aad6aa4d426"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OAYTSPINQD6HL6C5EYMECAYHIG/bundle.json","state_url":"https://pith.science/pith/OAYTSPINQD6HL6C5EYMECAYHIG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OAYTSPINQD6HL6C5EYMECAYHIG/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":"2026-05-31T07:32:58Z","links":{"resolver":"https://pith.science/pith/OAYTSPINQD6HL6C5EYMECAYHIG","bundle":"https://pith.science/pith/OAYTSPINQD6HL6C5EYMECAYHIG/bundle.json","state":"https://pith.science/pith/OAYTSPINQD6HL6C5EYMECAYHIG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OAYTSPINQD6HL6C5EYMECAYHIG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:OAYTSPINQD6HL6C5EYMECAYHIG","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":"82b6cc8819673c303dc4bced4e49e401c147a56c07e6fc892b6dedfabd9c5512","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-01-13T07:17:54Z","title_canon_sha256":"880af7c969987665ba95549c3fa49610231d9dd0408e373b45b83d7bf69e64bf"},"schema_version":"1.0","source":{"id":"1201.2749","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.2749","created_at":"2026-05-18T03:57:26Z"},{"alias_kind":"arxiv_version","alias_value":"1201.2749v3","created_at":"2026-05-18T03:57:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.2749","created_at":"2026-05-18T03:57:26Z"},{"alias_kind":"pith_short_12","alias_value":"OAYTSPINQD6H","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"OAYTSPINQD6HL6C5","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"OAYTSPIN","created_at":"2026-05-18T12:27:16Z"}],"graph_snapshots":[{"event_id":"sha256:9ba25d17f5e1631a6db358e8df6ce0437fa6d90e34ae731fa5d20aad6aa4d426","target":"graph","created_at":"2026-05-18T03:57:26Z","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":"The relaxation dynamics of the one-dimensional totally asymmetric simple exclusion process on a ring is considered in the case of step initial condition. Analyzing the time evolution of the local particle densities and currents by the Bethe ansatz method, we examine their full relaxation dynamics. As a result, we observe peculiar behaviors, such as the emergence of a ripple in the density profile and the existence of the excessive particle currents. Moreover, by making a finite-size scaling analysis of the asymptotic amplitudes of the local densities and currents, we find the scaling exponents","authors_text":"Jun Sato, Kazumitsu Sakai, Kohei Motegi","cross_cats":["math-ph","math.MP","nlin.SI"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-01-13T07:17:54Z","title":"Exact Relaxation Dynamics in the Totally Asymmetric Simple Exclusion Process"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.2749","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":"sha256:3c3e2684e8f10f65dba8dc847f096a04a8336003d590b8d50b294d2ede3c88cb","target":"record","created_at":"2026-05-18T03:57:26Z","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":"82b6cc8819673c303dc4bced4e49e401c147a56c07e6fc892b6dedfabd9c5512","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-01-13T07:17:54Z","title_canon_sha256":"880af7c969987665ba95549c3fa49610231d9dd0408e373b45b83d7bf69e64bf"},"schema_version":"1.0","source":{"id":"1201.2749","kind":"arxiv","version":3}},"canonical_sha256":"7031393d0d80fc75f85d261841030741abdcf4156afa124bfe17c25a71e9f69d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7031393d0d80fc75f85d261841030741abdcf4156afa124bfe17c25a71e9f69d","first_computed_at":"2026-05-18T03:57:26.621966Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:57:26.621966Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"u6gW35mJC6N85DyPcGXZuHRPEyTGnGdt+UGFFwa5y9k8/H7VmuwkLu9sy+t88tv8OA3DIJdSLIUbuesrVOLMDg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:57:26.622738Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.2749","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3c3e2684e8f10f65dba8dc847f096a04a8336003d590b8d50b294d2ede3c88cb","sha256:9ba25d17f5e1631a6db358e8df6ce0437fa6d90e34ae731fa5d20aad6aa4d426"],"state_sha256":"4a382abd1c398ee67f51021f2edc9e7a99bb3888cce94e4a73065a6e30fdde7e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AKq+TeInhzSU7ZXBARMNaGPVXELmNkP6ZtnId5D4i06dGuXqJW9KdNAIm4rAEtyowM83v+u3dCU7J2/brAQ4Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T07:32:58.348581Z","bundle_sha256":"82fb1337ac2cab9a2032870ac8a5bb06d4dafbed3e6fd2b0408e5aff01d75f52"}}