{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:AZVB3YJFOMVQQJQFVTDZRWWER3","short_pith_number":"pith:AZVB3YJF","schema_version":"1.0","canonical_sha256":"066a1de125732b082605acc798dac48eccd23501238fa13d09dfd230c777cbb3","source":{"kind":"arxiv","id":"1704.00394","version":2},"attestation_state":"computed","paper":{"title":"Growing length scale accompanying the vitrification: A perspective based on non-singular density fluctuations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"primary_cat":"cond-mat.soft","authors_text":"Akira Furukawa","submitted_at":"2017-04-03T00:40:14Z","abstract_excerpt":"In glass forming liquids close to the glass transition point, even a very slight increase in the macroscopic density results in a dramatic slowing down of the macroscopic relaxation. Concomitantly, the local density itself fluctuates in space. Therefore, one can imagine that even very small local density variations control the local glassy nature. Based on this perspective, a model for describing growing length scale accompanying the vitrification is introduced, in which we assume that in a subsystem whose density is above a certain threshold value, $\\rho_{\\rm c}$, owing to steric constraints,"},"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":"1704.00394","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-04-03T00:40:14Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"title_canon_sha256":"3f1f453360b79a3e26fcce214f3b29019f8580f0cf481e28e86c28298a2205c2","abstract_canon_sha256":"ea214862685aaf2222b7fe4b7bd2a043fab1cea2c58fc24213322d37dcf2210a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:55.070717Z","signature_b64":"yfHLcSSNN/ZvbDSYCDJfFxbB1KJc3fPmlNJej3+uHoJeMXoi4vFRmGMFnnaxNXQzVcZHMtYwR8h4/+rrDVNrAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"066a1de125732b082605acc798dac48eccd23501238fa13d09dfd230c777cbb3","last_reissued_at":"2026-05-18T00:21:55.069968Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:55.069968Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Growing length scale accompanying the vitrification: A perspective based on non-singular density fluctuations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"primary_cat":"cond-mat.soft","authors_text":"Akira Furukawa","submitted_at":"2017-04-03T00:40:14Z","abstract_excerpt":"In glass forming liquids close to the glass transition point, even a very slight increase in the macroscopic density results in a dramatic slowing down of the macroscopic relaxation. Concomitantly, the local density itself fluctuates in space. Therefore, one can imagine that even very small local density variations control the local glassy nature. Based on this perspective, a model for describing growing length scale accompanying the vitrification is introduced, in which we assume that in a subsystem whose density is above a certain threshold value, $\\rho_{\\rm c}$, owing to steric constraints,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.00394","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":"1704.00394","created_at":"2026-05-18T00:21:55.070096+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.00394v2","created_at":"2026-05-18T00:21:55.070096+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.00394","created_at":"2026-05-18T00:21:55.070096+00:00"},{"alias_kind":"pith_short_12","alias_value":"AZVB3YJFOMVQ","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_16","alias_value":"AZVB3YJFOMVQQJQF","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_8","alias_value":"AZVB3YJF","created_at":"2026-05-18T12:31:08.081275+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/AZVB3YJFOMVQQJQFVTDZRWWER3","json":"https://pith.science/pith/AZVB3YJFOMVQQJQFVTDZRWWER3.json","graph_json":"https://pith.science/api/pith-number/AZVB3YJFOMVQQJQFVTDZRWWER3/graph.json","events_json":"https://pith.science/api/pith-number/AZVB3YJFOMVQQJQFVTDZRWWER3/events.json","paper":"https://pith.science/paper/AZVB3YJF"},"agent_actions":{"view_html":"https://pith.science/pith/AZVB3YJFOMVQQJQFVTDZRWWER3","download_json":"https://pith.science/pith/AZVB3YJFOMVQQJQFVTDZRWWER3.json","view_paper":"https://pith.science/paper/AZVB3YJF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.00394&json=true","fetch_graph":"https://pith.science/api/pith-number/AZVB3YJFOMVQQJQFVTDZRWWER3/graph.json","fetch_events":"https://pith.science/api/pith-number/AZVB3YJFOMVQQJQFVTDZRWWER3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AZVB3YJFOMVQQJQFVTDZRWWER3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AZVB3YJFOMVQQJQFVTDZRWWER3/action/storage_attestation","attest_author":"https://pith.science/pith/AZVB3YJFOMVQQJQFVTDZRWWER3/action/author_attestation","sign_citation":"https://pith.science/pith/AZVB3YJFOMVQQJQFVTDZRWWER3/action/citation_signature","submit_replication":"https://pith.science/pith/AZVB3YJFOMVQQJQFVTDZRWWER3/action/replication_record"}},"created_at":"2026-05-18T00:21:55.070096+00:00","updated_at":"2026-05-18T00:21:55.070096+00:00"}