{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:ZV6LMGA5GWPTX2NSRUUWZRB7JO","short_pith_number":"pith:ZV6LMGA5","schema_version":"1.0","canonical_sha256":"cd7cb6181d359f3be9b28d296cc43f4ba0c8491279417c40dd3cc98cf664f8c7","source":{"kind":"arxiv","id":"1402.7003","version":1},"attestation_state":"computed","paper":{"title":"Percolation approach to glassy dynamics with continuously broken ergodicity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Annalisa Fierro, Antonio Coniglio, Jeferson J. Arenzon, Mauro Sellitto","submitted_at":"2014-02-27T18:34:29Z","abstract_excerpt":"We show that the relaxation dynamics near a glass transition with continuous ergodicity breaking can be endowed with a geometric interpretation based on percolation theory. At mean-field level this approach is consistent with the mode-coupling theory (MCT) of type-A liquid-glass transitions and allows to disentangle the universal and nonuniversal contributions to MCT relaxation exponents. Scaling predictions for the time correlation function are successfully tested in the F12 schematic model and facilitated spin systems on a Bethe lattice. Our approach immediately suggests the extension of MCT"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1402.7003","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-02-27T18:34:29Z","cross_cats_sorted":[],"title_canon_sha256":"ef07d7de5fcdfd866f3595f363d32c3bd0f15035f7164c10dfc1da60fbac4517","abstract_canon_sha256":"e2b0f07872b01d9d44b1b3b5e1e3f0e4bb0215b0110a261ab4c2c38eb16b58af"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:43:36.303784Z","signature_b64":"P7L0xF627tGnWSq1LSq9zeilBDV9uHze7rFpVKg+R+RQV4NQT8sSQELYHV0rJ2EGKrbHMyPhPQ+apL6S+5KiCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cd7cb6181d359f3be9b28d296cc43f4ba0c8491279417c40dd3cc98cf664f8c7","last_reissued_at":"2026-05-18T02:43:36.303168Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:43:36.303168Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Percolation approach to glassy dynamics with continuously broken ergodicity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Annalisa Fierro, Antonio Coniglio, Jeferson J. Arenzon, Mauro Sellitto","submitted_at":"2014-02-27T18:34:29Z","abstract_excerpt":"We show that the relaxation dynamics near a glass transition with continuous ergodicity breaking can be endowed with a geometric interpretation based on percolation theory. At mean-field level this approach is consistent with the mode-coupling theory (MCT) of type-A liquid-glass transitions and allows to disentangle the universal and nonuniversal contributions to MCT relaxation exponents. Scaling predictions for the time correlation function are successfully tested in the F12 schematic model and facilitated spin systems on a Bethe lattice. Our approach immediately suggests the extension of MCT"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.7003","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1402.7003","created_at":"2026-05-18T02:43:36.303249+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.7003v1","created_at":"2026-05-18T02:43:36.303249+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.7003","created_at":"2026-05-18T02:43:36.303249+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZV6LMGA5GWPT","created_at":"2026-05-18T12:28:59.999130+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZV6LMGA5GWPTX2NS","created_at":"2026-05-18T12:28:59.999130+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZV6LMGA5","created_at":"2026-05-18T12:28:59.999130+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZV6LMGA5GWPTX2NSRUUWZRB7JO","json":"https://pith.science/pith/ZV6LMGA5GWPTX2NSRUUWZRB7JO.json","graph_json":"https://pith.science/api/pith-number/ZV6LMGA5GWPTX2NSRUUWZRB7JO/graph.json","events_json":"https://pith.science/api/pith-number/ZV6LMGA5GWPTX2NSRUUWZRB7JO/events.json","paper":"https://pith.science/paper/ZV6LMGA5"},"agent_actions":{"view_html":"https://pith.science/pith/ZV6LMGA5GWPTX2NSRUUWZRB7JO","download_json":"https://pith.science/pith/ZV6LMGA5GWPTX2NSRUUWZRB7JO.json","view_paper":"https://pith.science/paper/ZV6LMGA5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.7003&json=true","fetch_graph":"https://pith.science/api/pith-number/ZV6LMGA5GWPTX2NSRUUWZRB7JO/graph.json","fetch_events":"https://pith.science/api/pith-number/ZV6LMGA5GWPTX2NSRUUWZRB7JO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZV6LMGA5GWPTX2NSRUUWZRB7JO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZV6LMGA5GWPTX2NSRUUWZRB7JO/action/storage_attestation","attest_author":"https://pith.science/pith/ZV6LMGA5GWPTX2NSRUUWZRB7JO/action/author_attestation","sign_citation":"https://pith.science/pith/ZV6LMGA5GWPTX2NSRUUWZRB7JO/action/citation_signature","submit_replication":"https://pith.science/pith/ZV6LMGA5GWPTX2NSRUUWZRB7JO/action/replication_record"}},"created_at":"2026-05-18T02:43:36.303249+00:00","updated_at":"2026-05-18T02:43:36.303249+00:00"}