{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:FXITJIZY367TFDTGQ6QSZEGAHO","short_pith_number":"pith:FXITJIZY","canonical_record":{"source":{"id":"cond-mat/0311518","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-11-22T11:57:41Z","cross_cats_sorted":[],"title_canon_sha256":"ee3ab1a5cd24b3a14f44b35c178ff078a1334e7b23fd13d04c92b98c6cdc46b3","abstract_canon_sha256":"2d2798fee347e4f0ee4e403c6e7007122569e299e0da03190cdd884c284a590f"},"schema_version":"1.0"},"canonical_sha256":"2dd134a338dfbf328e6687a12c90c03b9fd076519bc9bc7990d892288de969bc","source":{"kind":"arxiv","id":"cond-mat/0311518","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0311518","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0311518v1","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0311518","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"pith_short_12","alias_value":"FXITJIZY367T","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"FXITJIZY367TFDTG","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"FXITJIZY","created_at":"2026-05-18T12:25:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:FXITJIZY367TFDTGQ6QSZEGAHO","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0311518","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-11-22T11:57:41Z","cross_cats_sorted":[],"title_canon_sha256":"ee3ab1a5cd24b3a14f44b35c178ff078a1334e7b23fd13d04c92b98c6cdc46b3","abstract_canon_sha256":"2d2798fee347e4f0ee4e403c6e7007122569e299e0da03190cdd884c284a590f"},"schema_version":"1.0"},"canonical_sha256":"2dd134a338dfbf328e6687a12c90c03b9fd076519bc9bc7990d892288de969bc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:58.846115Z","signature_b64":"AY+o7ZiIAXWsH7HRlNc3HmBoxUU0mG8Y3HEWrFqjWHafPxPY56owkxg/umG7DtgmF60WwobqHNbsBe3HibKhDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2dd134a338dfbf328e6687a12c90c03b9fd076519bc9bc7990d892288de969bc","last_reissued_at":"2026-05-18T01:39:58.845646Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:58.845646Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0311518","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":"2026-05-18T01:39:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7sM0MjLDs0RPC0BB4Jsm/to98oDsrUKRn+9OILUsFE2IlrBWxn93A+WM+ujyjrEdambN/ERhxsvmOtny/zXzAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:56:52.917506Z"},"content_sha256":"d97df996ac19af78e129d24f22c6c8cebd9367bec6669c082e1180e9a54c8c26","schema_version":"1.0","event_id":"sha256:d97df996ac19af78e129d24f22c6c8cebd9367bec6669c082e1180e9a54c8c26"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:FXITJIZY367TFDTGQ6QSZEGAHO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Static- and dynamical-phase transition in one-dimensional reaction-diffusion systems with boundaries","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Amir Aghamohammadi, Mohammad Khorrami","submitted_at":"2003-11-22T11:57:41Z","abstract_excerpt":"A general system of particles (of one or several species) on a one dimensional lattice with boundaries is considered. Two general behaviors of such systems are investigated. The stationary behavior of the system, and the dominant way of the relaxation of the system toward its stationary system. Bases on the first behavior, static phase transitions (discontinuous changes in the stationary profiles of the system) are studied. Based on the second behavior, dynamical phase transitions (discontinuous changes in the relaxation-times of the system) are studied. The investigation is specialized on sys"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0311518","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":"2026-05-18T01:39:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VWrd2Kdd14CgZQtBghgoZaGpRNslXMDYrQM0IfsGgUbZAIevlACGTlQT5CpNRA8VqyQgbPlfZdN8RAUzMdW6Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:56:52.917858Z"},"content_sha256":"7868264ba4ceb9f68fc36be1a09b2a97e7dd360c6dde08226d9b6e8d9d2dfd00","schema_version":"1.0","event_id":"sha256:7868264ba4ceb9f68fc36be1a09b2a97e7dd360c6dde08226d9b6e8d9d2dfd00"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FXITJIZY367TFDTGQ6QSZEGAHO/bundle.json","state_url":"https://pith.science/pith/FXITJIZY367TFDTGQ6QSZEGAHO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FXITJIZY367TFDTGQ6QSZEGAHO/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":"2026-05-28T05:56:52Z","links":{"resolver":"https://pith.science/pith/FXITJIZY367TFDTGQ6QSZEGAHO","bundle":"https://pith.science/pith/FXITJIZY367TFDTGQ6QSZEGAHO/bundle.json","state":"https://pith.science/pith/FXITJIZY367TFDTGQ6QSZEGAHO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FXITJIZY367TFDTGQ6QSZEGAHO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:FXITJIZY367TFDTGQ6QSZEGAHO","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":"2d2798fee347e4f0ee4e403c6e7007122569e299e0da03190cdd884c284a590f","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-11-22T11:57:41Z","title_canon_sha256":"ee3ab1a5cd24b3a14f44b35c178ff078a1334e7b23fd13d04c92b98c6cdc46b3"},"schema_version":"1.0","source":{"id":"cond-mat/0311518","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0311518","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0311518v1","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0311518","created_at":"2026-05-18T01:39:58Z"},{"alias_kind":"pith_short_12","alias_value":"FXITJIZY367T","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"FXITJIZY367TFDTG","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"FXITJIZY","created_at":"2026-05-18T12:25:51Z"}],"graph_snapshots":[{"event_id":"sha256:7868264ba4ceb9f68fc36be1a09b2a97e7dd360c6dde08226d9b6e8d9d2dfd00","target":"graph","created_at":"2026-05-18T01:39:58Z","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":"A general system of particles (of one or several species) on a one dimensional lattice with boundaries is considered. Two general behaviors of such systems are investigated. The stationary behavior of the system, and the dominant way of the relaxation of the system toward its stationary system. Bases on the first behavior, static phase transitions (discontinuous changes in the stationary profiles of the system) are studied. Based on the second behavior, dynamical phase transitions (discontinuous changes in the relaxation-times of the system) are studied. The investigation is specialized on sys","authors_text":"Amir Aghamohammadi, Mohammad Khorrami","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-11-22T11:57:41Z","title":"Static- and dynamical-phase transition in one-dimensional reaction-diffusion systems with boundaries"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0311518","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:d97df996ac19af78e129d24f22c6c8cebd9367bec6669c082e1180e9a54c8c26","target":"record","created_at":"2026-05-18T01:39:58Z","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":"2d2798fee347e4f0ee4e403c6e7007122569e299e0da03190cdd884c284a590f","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-11-22T11:57:41Z","title_canon_sha256":"ee3ab1a5cd24b3a14f44b35c178ff078a1334e7b23fd13d04c92b98c6cdc46b3"},"schema_version":"1.0","source":{"id":"cond-mat/0311518","kind":"arxiv","version":1}},"canonical_sha256":"2dd134a338dfbf328e6687a12c90c03b9fd076519bc9bc7990d892288de969bc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2dd134a338dfbf328e6687a12c90c03b9fd076519bc9bc7990d892288de969bc","first_computed_at":"2026-05-18T01:39:58.845646Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:58.845646Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AY+o7ZiIAXWsH7HRlNc3HmBoxUU0mG8Y3HEWrFqjWHafPxPY56owkxg/umG7DtgmF60WwobqHNbsBe3HibKhDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:58.846115Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0311518","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d97df996ac19af78e129d24f22c6c8cebd9367bec6669c082e1180e9a54c8c26","sha256:7868264ba4ceb9f68fc36be1a09b2a97e7dd360c6dde08226d9b6e8d9d2dfd00"],"state_sha256":"5487f5c944ee5716b8f34a800ccc017a1b1501ec02abe155c17b05044b447d20"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CENuQpp//8HGxOS3DdpcPVrLY4mRGKE6W9ZfhmfAZntwiQugZzvFV00+UoRZC3SGTrSqfy9ZbNhsXwoz0uBNBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T05:56:52.919979Z","bundle_sha256":"310da3f10a3610a488e9a1b50bafc8cef3e8a23fac9c97a4bb6d8e934e14d109"}}