{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:TOKEZZ2YUZMUIXKUNGTH35TULW","short_pith_number":"pith:TOKEZZ2Y","schema_version":"1.0","canonical_sha256":"9b944ce758a659445d5469a67df6745da4612be90f5f6757ddbe323b813d2a0b","source":{"kind":"arxiv","id":"2406.15726","version":1},"attestation_state":"computed","paper":{"title":"Revisiting nonequilibrium characterization of glass: History dependence in solids","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"Koun Shirai","submitted_at":"2024-06-22T04:29:34Z","abstract_excerpt":"Glass has long been considered a nonequilibrium material. The primary reason is its history-dependent properties: the obtained properties are not uniquely determined by two state variables alone, namely, temperature and volume, but are affected by the process parameters, such as cooling rates. However, closer observations show that this history dependence is common in solid; in crystal growth, the properties of an obtained crystal are affected by the preparation conditions through defect structures and metallurgical structures. The problem with the previous reasoning of history dependence lies"},"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":"2406.15726","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2024-06-22T04:29:34Z","cross_cats_sorted":[],"title_canon_sha256":"7f9f2a879282be9eb12a8b130113c94605cf5110b47aba04b12d6312e973f8b4","abstract_canon_sha256":"ef6cab633c695f9ee729c61b392e4e8a3012875f2d0c75512d051fafd480d868"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:35:26.660693Z","signature_b64":"W8AHA0uANbTwCszTugS0laSCDBpiQX5c0xvFRUmtVlIroMVovUdKL6SFUK11E8Y8DfPAWkbwHEI8L9PlvPhNDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b944ce758a659445d5469a67df6745da4612be90f5f6757ddbe323b813d2a0b","last_reissued_at":"2026-07-05T08:35:26.660262Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:35:26.660262Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Revisiting nonequilibrium characterization of glass: History dependence in solids","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"Koun Shirai","submitted_at":"2024-06-22T04:29:34Z","abstract_excerpt":"Glass has long been considered a nonequilibrium material. The primary reason is its history-dependent properties: the obtained properties are not uniquely determined by two state variables alone, namely, temperature and volume, but are affected by the process parameters, such as cooling rates. However, closer observations show that this history dependence is common in solid; in crystal growth, the properties of an obtained crystal are affected by the preparation conditions through defect structures and metallurgical structures. The problem with the previous reasoning of history dependence lies"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.15726","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.15726/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2406.15726","created_at":"2026-07-05T08:35:26.660323+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.15726v1","created_at":"2026-07-05T08:35:26.660323+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.15726","created_at":"2026-07-05T08:35:26.660323+00:00"},{"alias_kind":"pith_short_12","alias_value":"TOKEZZ2YUZMU","created_at":"2026-07-05T08:35:26.660323+00:00"},{"alias_kind":"pith_short_16","alias_value":"TOKEZZ2YUZMUIXKU","created_at":"2026-07-05T08:35:26.660323+00:00"},{"alias_kind":"pith_short_8","alias_value":"TOKEZZ2Y","created_at":"2026-07-05T08:35:26.660323+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.20630","citing_title":"The total energy approach for calculating the specific heat of liquids and glasses","ref_index":56,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TOKEZZ2YUZMUIXKUNGTH35TULW","json":"https://pith.science/pith/TOKEZZ2YUZMUIXKUNGTH35TULW.json","graph_json":"https://pith.science/api/pith-number/TOKEZZ2YUZMUIXKUNGTH35TULW/graph.json","events_json":"https://pith.science/api/pith-number/TOKEZZ2YUZMUIXKUNGTH35TULW/events.json","paper":"https://pith.science/paper/TOKEZZ2Y"},"agent_actions":{"view_html":"https://pith.science/pith/TOKEZZ2YUZMUIXKUNGTH35TULW","download_json":"https://pith.science/pith/TOKEZZ2YUZMUIXKUNGTH35TULW.json","view_paper":"https://pith.science/paper/TOKEZZ2Y","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.15726&json=true","fetch_graph":"https://pith.science/api/pith-number/TOKEZZ2YUZMUIXKUNGTH35TULW/graph.json","fetch_events":"https://pith.science/api/pith-number/TOKEZZ2YUZMUIXKUNGTH35TULW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TOKEZZ2YUZMUIXKUNGTH35TULW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TOKEZZ2YUZMUIXKUNGTH35TULW/action/storage_attestation","attest_author":"https://pith.science/pith/TOKEZZ2YUZMUIXKUNGTH35TULW/action/author_attestation","sign_citation":"https://pith.science/pith/TOKEZZ2YUZMUIXKUNGTH35TULW/action/citation_signature","submit_replication":"https://pith.science/pith/TOKEZZ2YUZMUIXKUNGTH35TULW/action/replication_record"}},"created_at":"2026-07-05T08:35:26.660323+00:00","updated_at":"2026-07-05T08:35:26.660323+00:00"}