{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:5YDKFWOSG3B4XQLQ3ESP73YAIR","short_pith_number":"pith:5YDKFWOS","canonical_record":{"source":{"id":"1607.08267","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2016-07-27T21:20:52Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"e59a8520489cdea7a8248684e703057151b9c5804444cc30e86252bcbe939d6d","abstract_canon_sha256":"50bc69da8238930a188df68516d4967016f1cdd1bee3280e3063d6ddef954f78"},"schema_version":"1.0"},"canonical_sha256":"ee06a2d9d236c3cbc170d924ffef00445f89e6e321f6114d36ef153a4a441c83","source":{"kind":"arxiv","id":"1607.08267","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1607.08267","created_at":"2026-05-18T01:10:19Z"},{"alias_kind":"arxiv_version","alias_value":"1607.08267v1","created_at":"2026-05-18T01:10:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.08267","created_at":"2026-05-18T01:10:19Z"},{"alias_kind":"pith_short_12","alias_value":"5YDKFWOSG3B4","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5YDKFWOSG3B4XQLQ","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5YDKFWOS","created_at":"2026-05-18T12:30:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:5YDKFWOSG3B4XQLQ3ESP73YAIR","target":"record","payload":{"canonical_record":{"source":{"id":"1607.08267","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2016-07-27T21:20:52Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"e59a8520489cdea7a8248684e703057151b9c5804444cc30e86252bcbe939d6d","abstract_canon_sha256":"50bc69da8238930a188df68516d4967016f1cdd1bee3280e3063d6ddef954f78"},"schema_version":"1.0"},"canonical_sha256":"ee06a2d9d236c3cbc170d924ffef00445f89e6e321f6114d36ef153a4a441c83","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:10:19.540299Z","signature_b64":"0fhkFTkzM7Ds/PAmHqNOurQff6jrwAKdux4aYaVjwYapKwXzQWV+l8gpJLBxsM/eeOLtjXvxpo3ctxsQTdU9CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee06a2d9d236c3cbc170d924ffef00445f89e6e321f6114d36ef153a4a441c83","last_reissued_at":"2026-05-18T01:10:19.539816Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:10:19.539816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1607.08267","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":"2026-05-18T01:10:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3gdHeaPPGM9mq4a3Xbye6o3Nw6mfQTDY6+Gz9rjRdsFHORr3hC6ALfb+BJhsfMQ4pJywg+B5jNd7EMl23qJzDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T04:28:50.783779Z"},"content_sha256":"3882e723b938e6ca7e0abaaa7b6e400a262c8f5ec757cbd1a2672b029f0e795a","schema_version":"1.0","event_id":"sha256:3882e723b938e6ca7e0abaaa7b6e400a262c8f5ec757cbd1a2672b029f0e795a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:5YDKFWOSG3B4XQLQ3ESP73YAIR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Assessment of Predictor-Corrector strategy for the Burridge-Knopoff model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"math.NA","authors_text":"Corrado Mascia, Pierfrancesco Moschetta","submitted_at":"2016-07-27T21:20:52Z","abstract_excerpt":"A Predictor-Corrector strategy is employed for the numerical simulation of the one-dimensional Burridge-Knopoff model of earthquakes. This approach is totally explicit and allows to reproduce the main features of the model. The results achieved are compared with those of several previous works available in the literature, in order to state the effectiveness of the novel numerical strategy. Simulations are performed starting from the simplest cases and are aimed at studying the qualitative trends of the phenomena under analysis. By increasing the size of the associated differential system, it i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.08267","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":"2026-05-18T01:10:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IP1/DGYxYWHhPosMLapVTINX+d3pHYk9UQdUORS1bi3ptNojK9TTObaBjFhuvzHN3QtSxK3Wlq3B/ZLlGNTaAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T04:28:50.784487Z"},"content_sha256":"fe461452dbe3a14242d467006b2521c4e8e76d054dae128dda50a8f1cf4b6991","schema_version":"1.0","event_id":"sha256:fe461452dbe3a14242d467006b2521c4e8e76d054dae128dda50a8f1cf4b6991"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5YDKFWOSG3B4XQLQ3ESP73YAIR/bundle.json","state_url":"https://pith.science/pith/5YDKFWOSG3B4XQLQ3ESP73YAIR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5YDKFWOSG3B4XQLQ3ESP73YAIR/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":"2026-05-23T04:28:50Z","links":{"resolver":"https://pith.science/pith/5YDKFWOSG3B4XQLQ3ESP73YAIR","bundle":"https://pith.science/pith/5YDKFWOSG3B4XQLQ3ESP73YAIR/bundle.json","state":"https://pith.science/pith/5YDKFWOSG3B4XQLQ3ESP73YAIR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5YDKFWOSG3B4XQLQ3ESP73YAIR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:5YDKFWOSG3B4XQLQ3ESP73YAIR","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":"50bc69da8238930a188df68516d4967016f1cdd1bee3280e3063d6ddef954f78","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2016-07-27T21:20:52Z","title_canon_sha256":"e59a8520489cdea7a8248684e703057151b9c5804444cc30e86252bcbe939d6d"},"schema_version":"1.0","source":{"id":"1607.08267","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1607.08267","created_at":"2026-05-18T01:10:19Z"},{"alias_kind":"arxiv_version","alias_value":"1607.08267v1","created_at":"2026-05-18T01:10:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.08267","created_at":"2026-05-18T01:10:19Z"},{"alias_kind":"pith_short_12","alias_value":"5YDKFWOSG3B4","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5YDKFWOSG3B4XQLQ","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5YDKFWOS","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:fe461452dbe3a14242d467006b2521c4e8e76d054dae128dda50a8f1cf4b6991","target":"graph","created_at":"2026-05-18T01:10:19Z","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 Predictor-Corrector strategy is employed for the numerical simulation of the one-dimensional Burridge-Knopoff model of earthquakes. This approach is totally explicit and allows to reproduce the main features of the model. The results achieved are compared with those of several previous works available in the literature, in order to state the effectiveness of the novel numerical strategy. Simulations are performed starting from the simplest cases and are aimed at studying the qualitative trends of the phenomena under analysis. By increasing the size of the associated differential system, it i","authors_text":"Corrado Mascia, Pierfrancesco Moschetta","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2016-07-27T21:20:52Z","title":"Assessment of Predictor-Corrector strategy for the Burridge-Knopoff model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.08267","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":"sha256:3882e723b938e6ca7e0abaaa7b6e400a262c8f5ec757cbd1a2672b029f0e795a","target":"record","created_at":"2026-05-18T01:10:19Z","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":"50bc69da8238930a188df68516d4967016f1cdd1bee3280e3063d6ddef954f78","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2016-07-27T21:20:52Z","title_canon_sha256":"e59a8520489cdea7a8248684e703057151b9c5804444cc30e86252bcbe939d6d"},"schema_version":"1.0","source":{"id":"1607.08267","kind":"arxiv","version":1}},"canonical_sha256":"ee06a2d9d236c3cbc170d924ffef00445f89e6e321f6114d36ef153a4a441c83","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ee06a2d9d236c3cbc170d924ffef00445f89e6e321f6114d36ef153a4a441c83","first_computed_at":"2026-05-18T01:10:19.539816Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:10:19.539816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0fhkFTkzM7Ds/PAmHqNOurQff6jrwAKdux4aYaVjwYapKwXzQWV+l8gpJLBxsM/eeOLtjXvxpo3ctxsQTdU9CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:10:19.540299Z","signed_message":"canonical_sha256_bytes"},"source_id":"1607.08267","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3882e723b938e6ca7e0abaaa7b6e400a262c8f5ec757cbd1a2672b029f0e795a","sha256:fe461452dbe3a14242d467006b2521c4e8e76d054dae128dda50a8f1cf4b6991"],"state_sha256":"0ff685144bf4c6012719d3788d7359006fbafb31a98f5160da2e8ddbc8c1f720"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"98gnwVGYSXi3Pz86hnVpjm/umBSeDhH6bczgju27pkhlQrflmQ60j3HbTxpihCcCdL73tXj8aCGFo0uxM51gCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T04:28:50.788256Z","bundle_sha256":"290a7cc32d9ff53805b71fe79459a4667124460589c3cd3f6ba0c2e183544fed"}}