{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:2B5N6RW7F76COWXWJKVIPHCJB4","short_pith_number":"pith:2B5N6RW7","schema_version":"1.0","canonical_sha256":"d07adf46df2ffc275af64aaa879c490f399fe036df3bc0023fc417e87087016b","source":{"kind":"arxiv","id":"1407.5677","version":2},"attestation_state":"computed","paper":{"title":"Hopping and the Stokes-Einstein relation breakdown in simple glass formers","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"Francesco Zamponi, Giorgio Parisi, Patrick Charbonneau, Yuliang Jin","submitted_at":"2014-07-21T22:14:33Z","abstract_excerpt":"One of the most actively debated issues in the study of the glass transition is whether a mean-field description is a reasonable starting point for understanding experimental glass formers. Although the mean-field theory of the glass transition -- like that of other statistical systems -- is exact when the spatial dimension $d\\rightarrow\\infty$, the evolution of systems properties with $d$ may not be smooth. Finite-dimensional effects could dramatically change what happens in physical dimensions, $d=2,3$. For standard phase transitions finite-dimensional effects are typically captured by renor"},"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":"1407.5677","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-07-21T22:14:33Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"0470758e611662cfb221f903b4a732004b01c2a3950567832bc8132c6d7c5cb5","abstract_canon_sha256":"be0e59008dda40c9f5f253cd150177c70e00a768319227a0d81f8f9869fb4eaf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:39:31.668731Z","signature_b64":"nWYqJz19JfwAFqbqJ0I4CeS5qbIIbw1VcZffKELy5KZO7NhWJ2teFVCHBaz8skphBLFheF8mZu1L68t6k760AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d07adf46df2ffc275af64aaa879c490f399fe036df3bc0023fc417e87087016b","last_reissued_at":"2026-05-18T02:39:31.668234Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:39:31.668234Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hopping and the Stokes-Einstein relation breakdown in simple glass formers","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"Francesco Zamponi, Giorgio Parisi, Patrick Charbonneau, Yuliang Jin","submitted_at":"2014-07-21T22:14:33Z","abstract_excerpt":"One of the most actively debated issues in the study of the glass transition is whether a mean-field description is a reasonable starting point for understanding experimental glass formers. Although the mean-field theory of the glass transition -- like that of other statistical systems -- is exact when the spatial dimension $d\\rightarrow\\infty$, the evolution of systems properties with $d$ may not be smooth. Finite-dimensional effects could dramatically change what happens in physical dimensions, $d=2,3$. For standard phase transitions finite-dimensional effects are typically captured by renor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.5677","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1407.5677","created_at":"2026-05-18T02:39:31.668308+00:00"},{"alias_kind":"arxiv_version","alias_value":"1407.5677v2","created_at":"2026-05-18T02:39:31.668308+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.5677","created_at":"2026-05-18T02:39:31.668308+00:00"},{"alias_kind":"pith_short_12","alias_value":"2B5N6RW7F76C","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_16","alias_value":"2B5N6RW7F76COWXW","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_8","alias_value":"2B5N6RW7","created_at":"2026-05-18T12:28:09.283467+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/2B5N6RW7F76COWXWJKVIPHCJB4","json":"https://pith.science/pith/2B5N6RW7F76COWXWJKVIPHCJB4.json","graph_json":"https://pith.science/api/pith-number/2B5N6RW7F76COWXWJKVIPHCJB4/graph.json","events_json":"https://pith.science/api/pith-number/2B5N6RW7F76COWXWJKVIPHCJB4/events.json","paper":"https://pith.science/paper/2B5N6RW7"},"agent_actions":{"view_html":"https://pith.science/pith/2B5N6RW7F76COWXWJKVIPHCJB4","download_json":"https://pith.science/pith/2B5N6RW7F76COWXWJKVIPHCJB4.json","view_paper":"https://pith.science/paper/2B5N6RW7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1407.5677&json=true","fetch_graph":"https://pith.science/api/pith-number/2B5N6RW7F76COWXWJKVIPHCJB4/graph.json","fetch_events":"https://pith.science/api/pith-number/2B5N6RW7F76COWXWJKVIPHCJB4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2B5N6RW7F76COWXWJKVIPHCJB4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2B5N6RW7F76COWXWJKVIPHCJB4/action/storage_attestation","attest_author":"https://pith.science/pith/2B5N6RW7F76COWXWJKVIPHCJB4/action/author_attestation","sign_citation":"https://pith.science/pith/2B5N6RW7F76COWXWJKVIPHCJB4/action/citation_signature","submit_replication":"https://pith.science/pith/2B5N6RW7F76COWXWJKVIPHCJB4/action/replication_record"}},"created_at":"2026-05-18T02:39:31.668308+00:00","updated_at":"2026-05-18T02:39:31.668308+00:00"}