{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:LE3TKBNE3JH5TR7QXZ44PUYPHU","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":"ce0a113a060e463258209e413924b390bf4bc2d5a86c60d46e3164f24b303d75","cross_cats_sorted":["cond-mat.stat-mech","nlin.AO","physics.soc-ph","stat.ME"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cs.SI","submitted_at":"2016-08-22T15:33:16Z","title_canon_sha256":"42c22151073a1a523bcf109885a370a8644c4f86bafb7d584edf5e46ffaaa8f1"},"schema_version":"1.0","source":{"id":"1608.06196","kind":"arxiv","version":5}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.06196","created_at":"2026-07-05T01:00:29Z"},{"alias_kind":"arxiv_version","alias_value":"1608.06196v5","created_at":"2026-07-05T01:00:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.06196","created_at":"2026-07-05T01:00:29Z"},{"alias_kind":"pith_short_12","alias_value":"LE3TKBNE3JH5","created_at":"2026-07-05T01:00:29Z"},{"alias_kind":"pith_short_16","alias_value":"LE3TKBNE3JH5TR7Q","created_at":"2026-07-05T01:00:29Z"},{"alias_kind":"pith_short_8","alias_value":"LE3TKBNE","created_at":"2026-07-05T01:00:29Z"}],"graph_snapshots":[{"event_id":"sha256:f07d70a2d8567e45dd7ededf85cabee83a7595291c3d696873be114d6e4198a3","target":"graph","created_at":"2026-07-05T01:00:29Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/1608.06196/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Multilayer networks allow one to represent diverse and coupled connectivity patterns --- e.g., time-dependence, multiple subsystems, or both --- that arise in many applications and which are difficult or awkward to incorporate into standard network representations. In the study of multilayer networks, it is important to investigate mesoscale (i.e., intermediate-scale) structures, such as dense sets of nodes known as communities, to discover network features that are not apparent at the microscale or the macroscale. The ill-defined nature of mesoscale structure and its ubiquity in empirical net","authors_text":"Alex Arenas, Lucas G. S. Jeub, Marya Bazzi, Mason A. Porter, Sam D. Howison","cross_cats":["cond-mat.stat-mech","nlin.AO","physics.soc-ph","stat.ME"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cs.SI","submitted_at":"2016-08-22T15:33:16Z","title":"A Framework for the Construction of Generative Models for Mesoscale Structure in Multilayer Networks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.06196","kind":"arxiv","version":5},"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:ea011219bfb9544a096770ec55986ca0cde475e6df1263838685aaafa4b8a54a","target":"record","created_at":"2026-07-05T01:00:29Z","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":"ce0a113a060e463258209e413924b390bf4bc2d5a86c60d46e3164f24b303d75","cross_cats_sorted":["cond-mat.stat-mech","nlin.AO","physics.soc-ph","stat.ME"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cs.SI","submitted_at":"2016-08-22T15:33:16Z","title_canon_sha256":"42c22151073a1a523bcf109885a370a8644c4f86bafb7d584edf5e46ffaaa8f1"},"schema_version":"1.0","source":{"id":"1608.06196","kind":"arxiv","version":5}},"canonical_sha256":"59373505a4da4fd9c7f0be79c7d30f3d0bf6149d969ed8905d84fb8922e04bca","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"59373505a4da4fd9c7f0be79c7d30f3d0bf6149d969ed8905d84fb8922e04bca","first_computed_at":"2026-07-05T01:00:29.926205Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:00:29.926205Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kQsRJzACbkqanQC5gvNIf1XKGIjG4muJYijgbQxwqG5FZz6Ga2c+viDAClEHFRpb9HX/GWV6NkywD8g73pqIDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T01:00:29.926772Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.06196","source_kind":"arxiv","source_version":5}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ea011219bfb9544a096770ec55986ca0cde475e6df1263838685aaafa4b8a54a","sha256:f07d70a2d8567e45dd7ededf85cabee83a7595291c3d696873be114d6e4198a3"],"state_sha256":"29f713863bb3b1a29fbd279f6950e7b61c42700ecb4d69a955c0a2e9cef22f42"}