{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:YQY35LWKETZIXEQ5FVJMCU2AQS","short_pith_number":"pith:YQY35LWK","schema_version":"1.0","canonical_sha256":"c431beaeca24f28b921d2d52c1534084ab7b45492601da8dfb3afda89d7f85cc","source":{"kind":"arxiv","id":"cond-mat/9901271","version":2},"attestation_state":"computed","paper":{"title":"Crossover to Potential Energy Landscape Dominated Dynamics in a Model Glass-forming Liquid","license":"","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"primary_cat":"cond-mat.soft","authors_text":"Jeppe C. Dyre, Sharon C. Glotzer, Srikanth Sastry, Thomas B. Schroeder","submitted_at":"1999-01-25T19:47:17Z","abstract_excerpt":"An equilibrated model glass-forming liquid is studied by mapping successive configurations produced by molecular dynamics simulation onto a time series of inherent structures (local minima in the potential energy). Using this ``inherent dynamics'' approach we find direct numerical evidence for the long held view that below a crossover temperature, $T_x$, the liquid's dynamics can be separated into (i) vibrations around inherent structures and (ii) transitions between inherent structures (M. Goldstein, J. Chem. Phys. {\\bf 51}, 3728 (1969)), i.e., the dynamics become ``dominated'' by the potenti"},"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":"cond-mat/9901271","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.soft","submitted_at":"1999-01-25T19:47:17Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"title_canon_sha256":"2269fa6053e719f96193c39f8da489030f42caf51c06d8d81cb8e215d0af03a7","abstract_canon_sha256":"cb38d440084c9220999b7f0497a0e0f0e4e8f1ae4e83b5aaf9eebb992d2df70c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:59:14.246640Z","signature_b64":"4EQk7Yo5+QfhEtau/m5vdQ+0dU2N8wpSK9KsZDTHzgPoDxKcphclkI+M7KWkYQThy8liqGTCEU9BXdBWOhNjBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c431beaeca24f28b921d2d52c1534084ab7b45492601da8dfb3afda89d7f85cc","last_reissued_at":"2026-05-18T03:59:14.245870Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:59:14.245870Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Crossover to Potential Energy Landscape Dominated Dynamics in a Model Glass-forming Liquid","license":"","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"primary_cat":"cond-mat.soft","authors_text":"Jeppe C. Dyre, Sharon C. Glotzer, Srikanth Sastry, Thomas B. Schroeder","submitted_at":"1999-01-25T19:47:17Z","abstract_excerpt":"An equilibrated model glass-forming liquid is studied by mapping successive configurations produced by molecular dynamics simulation onto a time series of inherent structures (local minima in the potential energy). Using this ``inherent dynamics'' approach we find direct numerical evidence for the long held view that below a crossover temperature, $T_x$, the liquid's dynamics can be separated into (i) vibrations around inherent structures and (ii) transitions between inherent structures (M. Goldstein, J. Chem. Phys. {\\bf 51}, 3728 (1969)), i.e., the dynamics become ``dominated'' by the potenti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9901271","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":"cond-mat/9901271","created_at":"2026-05-18T03:59:14.245987+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9901271v2","created_at":"2026-05-18T03:59:14.245987+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9901271","created_at":"2026-05-18T03:59:14.245987+00:00"},{"alias_kind":"pith_short_12","alias_value":"YQY35LWKETZI","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"YQY35LWKETZIXEQ5","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"YQY35LWK","created_at":"2026-05-18T12:25:49.631198+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/YQY35LWKETZIXEQ5FVJMCU2AQS","json":"https://pith.science/pith/YQY35LWKETZIXEQ5FVJMCU2AQS.json","graph_json":"https://pith.science/api/pith-number/YQY35LWKETZIXEQ5FVJMCU2AQS/graph.json","events_json":"https://pith.science/api/pith-number/YQY35LWKETZIXEQ5FVJMCU2AQS/events.json","paper":"https://pith.science/paper/YQY35LWK"},"agent_actions":{"view_html":"https://pith.science/pith/YQY35LWKETZIXEQ5FVJMCU2AQS","download_json":"https://pith.science/pith/YQY35LWKETZIXEQ5FVJMCU2AQS.json","view_paper":"https://pith.science/paper/YQY35LWK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9901271&json=true","fetch_graph":"https://pith.science/api/pith-number/YQY35LWKETZIXEQ5FVJMCU2AQS/graph.json","fetch_events":"https://pith.science/api/pith-number/YQY35LWKETZIXEQ5FVJMCU2AQS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YQY35LWKETZIXEQ5FVJMCU2AQS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YQY35LWKETZIXEQ5FVJMCU2AQS/action/storage_attestation","attest_author":"https://pith.science/pith/YQY35LWKETZIXEQ5FVJMCU2AQS/action/author_attestation","sign_citation":"https://pith.science/pith/YQY35LWKETZIXEQ5FVJMCU2AQS/action/citation_signature","submit_replication":"https://pith.science/pith/YQY35LWKETZIXEQ5FVJMCU2AQS/action/replication_record"}},"created_at":"2026-05-18T03:59:14.245987+00:00","updated_at":"2026-05-18T03:59:14.245987+00:00"}