{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:B5KYXMT5EHQ6PADOSHWN57FGSI","short_pith_number":"pith:B5KYXMT5","canonical_record":{"source":{"id":"1001.2251","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2010-01-13T18:32:16Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"dc01328a680d75901c48913d770a6d8dff615e28ed33ce53d8a21a8a9c7b6ff8","abstract_canon_sha256":"7794a8d28fa36576064d02b189f0090342663f991358fd6858ad05bccd9e5e95"},"schema_version":"1.0"},"canonical_sha256":"0f558bb27d21e1e7806e91ecdefca69208a9005c218185bfa823cfbc282604f8","source":{"kind":"arxiv","id":"1001.2251","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1001.2251","created_at":"2026-05-18T03:23:49Z"},{"alias_kind":"arxiv_version","alias_value":"1001.2251v2","created_at":"2026-05-18T03:23:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.2251","created_at":"2026-05-18T03:23:49Z"},{"alias_kind":"pith_short_12","alias_value":"B5KYXMT5EHQ6","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_16","alias_value":"B5KYXMT5EHQ6PADO","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_8","alias_value":"B5KYXMT5","created_at":"2026-05-18T12:26:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:B5KYXMT5EHQ6PADOSHWN57FGSI","target":"record","payload":{"canonical_record":{"source":{"id":"1001.2251","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2010-01-13T18:32:16Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"dc01328a680d75901c48913d770a6d8dff615e28ed33ce53d8a21a8a9c7b6ff8","abstract_canon_sha256":"7794a8d28fa36576064d02b189f0090342663f991358fd6858ad05bccd9e5e95"},"schema_version":"1.0"},"canonical_sha256":"0f558bb27d21e1e7806e91ecdefca69208a9005c218185bfa823cfbc282604f8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:49.524604Z","signature_b64":"fOH2nlRIDBEbyFiViAIWb+2djqyKXrS4fXHolEmoPhk7jBMxkpK/3JX2426s+FhdsZh6szuRJJAaedfSNVWwCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0f558bb27d21e1e7806e91ecdefca69208a9005c218185bfa823cfbc282604f8","last_reissued_at":"2026-05-18T03:23:49.524075Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:49.524075Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1001.2251","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:23:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NFqAI8DZpSlMjKHdmVyajvFLsNCx5Vq0o/1HpVNAaLUPouTfrz3a4ydfNj3IRdM2HBU34tv++redJfDBdPFDDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T17:49:28.098912Z"},"content_sha256":"817174d503223dee2c3b7bb39bb69ca5ec5e1d30813f0c20b1f0a3c17fd2b3e7","schema_version":"1.0","event_id":"sha256:817174d503223dee2c3b7bb39bb69ca5ec5e1d30813f0c20b1f0a3c17fd2b3e7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:B5KYXMT5EHQ6PADOSHWN57FGSI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Lattice splitting under intermittent flows","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"physics.soc-ph","authors_text":"Konstantinos Trantopoulos, Markus Schl\\\"apfer","submitted_at":"2010-01-13T18:32:16Z","abstract_excerpt":"We study the splitting of regular square lattices subject to stochastic intermittent flows. Various flow patterns are produced by different groupings of the nodes, based on their random alternation between two possible states. The resulting flows on the lattices decrease with the number of groups according to a power law. By Monte Carlo simulations we reveal how the time span until the occurrence of a splitting depends on the flow patterns. Increasing the flow fluctuation frequency shortens this time span which reaches a minimum before rising again due to inertia effects incorporated in the mo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.2251","kind":"arxiv","version":2},"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":"2026-05-18T03:23:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6YkGs7WXVJFCPsYtNjBKszwzEfdiqIbiLt7W3vyYQoUsPZvUrx8s9hY4LAVGSYT8BqSGGqhLy8lSe/mnYshFAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T17:49:28.099292Z"},"content_sha256":"d299633dcafbf9bd39e04854f451eafd9ec97c172425c0db124d4d73df46793e","schema_version":"1.0","event_id":"sha256:d299633dcafbf9bd39e04854f451eafd9ec97c172425c0db124d4d73df46793e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/B5KYXMT5EHQ6PADOSHWN57FGSI/bundle.json","state_url":"https://pith.science/pith/B5KYXMT5EHQ6PADOSHWN57FGSI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/B5KYXMT5EHQ6PADOSHWN57FGSI/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":"2026-05-29T17:49:28Z","links":{"resolver":"https://pith.science/pith/B5KYXMT5EHQ6PADOSHWN57FGSI","bundle":"https://pith.science/pith/B5KYXMT5EHQ6PADOSHWN57FGSI/bundle.json","state":"https://pith.science/pith/B5KYXMT5EHQ6PADOSHWN57FGSI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/B5KYXMT5EHQ6PADOSHWN57FGSI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:B5KYXMT5EHQ6PADOSHWN57FGSI","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":"7794a8d28fa36576064d02b189f0090342663f991358fd6858ad05bccd9e5e95","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2010-01-13T18:32:16Z","title_canon_sha256":"dc01328a680d75901c48913d770a6d8dff615e28ed33ce53d8a21a8a9c7b6ff8"},"schema_version":"1.0","source":{"id":"1001.2251","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1001.2251","created_at":"2026-05-18T03:23:49Z"},{"alias_kind":"arxiv_version","alias_value":"1001.2251v2","created_at":"2026-05-18T03:23:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.2251","created_at":"2026-05-18T03:23:49Z"},{"alias_kind":"pith_short_12","alias_value":"B5KYXMT5EHQ6","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_16","alias_value":"B5KYXMT5EHQ6PADO","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_8","alias_value":"B5KYXMT5","created_at":"2026-05-18T12:26:05Z"}],"graph_snapshots":[{"event_id":"sha256:d299633dcafbf9bd39e04854f451eafd9ec97c172425c0db124d4d73df46793e","target":"graph","created_at":"2026-05-18T03:23:49Z","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 study the splitting of regular square lattices subject to stochastic intermittent flows. Various flow patterns are produced by different groupings of the nodes, based on their random alternation between two possible states. The resulting flows on the lattices decrease with the number of groups according to a power law. By Monte Carlo simulations we reveal how the time span until the occurrence of a splitting depends on the flow patterns. Increasing the flow fluctuation frequency shortens this time span which reaches a minimum before rising again due to inertia effects incorporated in the mo","authors_text":"Konstantinos Trantopoulos, Markus Schl\\\"apfer","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2010-01-13T18:32:16Z","title":"Lattice splitting under intermittent flows"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.2251","kind":"arxiv","version":2},"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":"sha256:817174d503223dee2c3b7bb39bb69ca5ec5e1d30813f0c20b1f0a3c17fd2b3e7","target":"record","created_at":"2026-05-18T03:23:49Z","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":"7794a8d28fa36576064d02b189f0090342663f991358fd6858ad05bccd9e5e95","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2010-01-13T18:32:16Z","title_canon_sha256":"dc01328a680d75901c48913d770a6d8dff615e28ed33ce53d8a21a8a9c7b6ff8"},"schema_version":"1.0","source":{"id":"1001.2251","kind":"arxiv","version":2}},"canonical_sha256":"0f558bb27d21e1e7806e91ecdefca69208a9005c218185bfa823cfbc282604f8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0f558bb27d21e1e7806e91ecdefca69208a9005c218185bfa823cfbc282604f8","first_computed_at":"2026-05-18T03:23:49.524075Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:23:49.524075Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fOH2nlRIDBEbyFiViAIWb+2djqyKXrS4fXHolEmoPhk7jBMxkpK/3JX2426s+FhdsZh6szuRJJAaedfSNVWwCw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:23:49.524604Z","signed_message":"canonical_sha256_bytes"},"source_id":"1001.2251","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:817174d503223dee2c3b7bb39bb69ca5ec5e1d30813f0c20b1f0a3c17fd2b3e7","sha256:d299633dcafbf9bd39e04854f451eafd9ec97c172425c0db124d4d73df46793e"],"state_sha256":"305453ed2ff2ec250138ca3c24cb6a4e228e0c576760cf600cfbd630b0fc7a19"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wM7ECQ8p9wc8rRu+n94L3C3qXdT0IliZ98KU8WLmKIyqqZnTuRZDhgsr6kNJVA5dw+BRlZjN+7umDfIXrcn7Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T17:49:28.102567Z","bundle_sha256":"1a2d7e7ac329e83bc4246723864d59d65e2f17fceba146e2cfebe8f2e5d2fe89"}}