{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:4DXRGG4UV5S4PXOKQYFZUBNG3U","short_pith_number":"pith:4DXRGG4U","schema_version":"1.0","canonical_sha256":"e0ef131b94af65c7ddca860b9a05a6dd19ceb18a6a51958f74cb68fcc91cb0c8","source":{"kind":"arxiv","id":"1504.05751","version":2},"attestation_state":"computed","paper":{"title":"The local atomic packing of a single-component glass is quasi-crystalline","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Farid F. Abraham","submitted_at":"2015-04-22T12:07:39Z","abstract_excerpt":"Our earlier Monte Carlo simulations of metastable supercooled-liquid and glass phases of Lennard-Jones atoms found several distinct signatures for identifying the glass transition boundary; i.e., the density, enthalpy, and pair distribution function dependences on temperature and pressure are different for the two phases (F. F. Abraham, J. Chem. Phys., 72, 359 (1980)). In this extension of that study, we base our analysis on the Ackland-Jones (A-J) method for determining the local crystal packing about each atom (G. Ackland & A. Jones, PRB 73, 054104 (2006)). It focuses on the angular distribu"},"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":"1504.05751","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2015-04-22T12:07:39Z","cross_cats_sorted":[],"title_canon_sha256":"bba89ea2dd254cceec79542303b3dbd68f0a39cf19d10d62d4e6ef9eb90fa14b","abstract_canon_sha256":"a0b1d9c864c27d998dd5c9a7e3f7b0531070e65e47540da728076b7c25eacd8f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:17:10.800107Z","signature_b64":"SNeWq1f5ypMA92mk3XFeFm8ni/tGfI9AQMOlZIv7wSkGKrz8EM9VjcVFf80Ug4fLtmDRF99xNphRQ9exy4sSCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e0ef131b94af65c7ddca860b9a05a6dd19ceb18a6a51958f74cb68fcc91cb0c8","last_reissued_at":"2026-05-18T02:17:10.799220Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:17:10.799220Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The local atomic packing of a single-component glass is quasi-crystalline","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Farid F. Abraham","submitted_at":"2015-04-22T12:07:39Z","abstract_excerpt":"Our earlier Monte Carlo simulations of metastable supercooled-liquid and glass phases of Lennard-Jones atoms found several distinct signatures for identifying the glass transition boundary; i.e., the density, enthalpy, and pair distribution function dependences on temperature and pressure are different for the two phases (F. F. Abraham, J. Chem. Phys., 72, 359 (1980)). In this extension of that study, we base our analysis on the Ackland-Jones (A-J) method for determining the local crystal packing about each atom (G. Ackland & A. Jones, PRB 73, 054104 (2006)). It focuses on the angular distribu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.05751","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":"1504.05751","created_at":"2026-05-18T02:17:10.799416+00:00"},{"alias_kind":"arxiv_version","alias_value":"1504.05751v2","created_at":"2026-05-18T02:17:10.799416+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.05751","created_at":"2026-05-18T02:17:10.799416+00:00"},{"alias_kind":"pith_short_12","alias_value":"4DXRGG4UV5S4","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_16","alias_value":"4DXRGG4UV5S4PXOK","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_8","alias_value":"4DXRGG4U","created_at":"2026-05-18T12:29:05.191682+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/4DXRGG4UV5S4PXOKQYFZUBNG3U","json":"https://pith.science/pith/4DXRGG4UV5S4PXOKQYFZUBNG3U.json","graph_json":"https://pith.science/api/pith-number/4DXRGG4UV5S4PXOKQYFZUBNG3U/graph.json","events_json":"https://pith.science/api/pith-number/4DXRGG4UV5S4PXOKQYFZUBNG3U/events.json","paper":"https://pith.science/paper/4DXRGG4U"},"agent_actions":{"view_html":"https://pith.science/pith/4DXRGG4UV5S4PXOKQYFZUBNG3U","download_json":"https://pith.science/pith/4DXRGG4UV5S4PXOKQYFZUBNG3U.json","view_paper":"https://pith.science/paper/4DXRGG4U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1504.05751&json=true","fetch_graph":"https://pith.science/api/pith-number/4DXRGG4UV5S4PXOKQYFZUBNG3U/graph.json","fetch_events":"https://pith.science/api/pith-number/4DXRGG4UV5S4PXOKQYFZUBNG3U/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4DXRGG4UV5S4PXOKQYFZUBNG3U/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4DXRGG4UV5S4PXOKQYFZUBNG3U/action/storage_attestation","attest_author":"https://pith.science/pith/4DXRGG4UV5S4PXOKQYFZUBNG3U/action/author_attestation","sign_citation":"https://pith.science/pith/4DXRGG4UV5S4PXOKQYFZUBNG3U/action/citation_signature","submit_replication":"https://pith.science/pith/4DXRGG4UV5S4PXOKQYFZUBNG3U/action/replication_record"}},"created_at":"2026-05-18T02:17:10.799416+00:00","updated_at":"2026-05-18T02:17:10.799416+00:00"}