{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:NKUNMOBBX3PWLD6PN4KOOPT6TB","short_pith_number":"pith:NKUNMOBB","schema_version":"1.0","canonical_sha256":"6aa8d63821bedf658fcf6f14e73e7e9852ebf22ceac5d8fb4c437212c77f5c07","source":{"kind":"arxiv","id":"1405.7389","version":1},"attestation_state":"computed","paper":{"title":"Local structure of supercritical matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.soft"],"primary_cat":"cond-mat.stat-mech","authors_text":"Dima Bolmatov, D. Zav'yalov, M. Zhernenkov","submitted_at":"2014-05-28T20:21:56Z","abstract_excerpt":"The supercritical state is currently viewed as uniform on the pressure-temperature phase diagram. Supercritical fluids have the dynamic motions of a gas but are able to dissolve materials like a liquid. They have started to be deployed in many important industrial applications stimulating fundamental theoretical work and development of experimental techniques. Here, we have studied local structure of supercritical matter by calculating static structure factor, mean force potential, self-diffusion, first coordination shell number and pair distribution function within very wide temperature range"},"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":"1405.7389","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-05-28T20:21:56Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.soft"],"title_canon_sha256":"bda2bacdc897ecc07e9e10d0f1729cfb45b87fb0a00dafcff70acb23cc956bc3","abstract_canon_sha256":"67c83e572ad405af3ae569fff316909566959b6cd22cf37b7ecef5e16494b758"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:50:51.341007Z","signature_b64":"3/NGP70lXwnCyu15QG9FyBfy3tl3/Lob2JU/NYJPEoeTRO9JS53bv39Vwg3r5XLcQv5j46liHWgxaiAMDW6GBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6aa8d63821bedf658fcf6f14e73e7e9852ebf22ceac5d8fb4c437212c77f5c07","last_reissued_at":"2026-05-18T02:50:51.340513Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:50:51.340513Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Local structure of supercritical matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.mtrl-sci","cond-mat.soft"],"primary_cat":"cond-mat.stat-mech","authors_text":"Dima Bolmatov, D. Zav'yalov, M. Zhernenkov","submitted_at":"2014-05-28T20:21:56Z","abstract_excerpt":"The supercritical state is currently viewed as uniform on the pressure-temperature phase diagram. Supercritical fluids have the dynamic motions of a gas but are able to dissolve materials like a liquid. They have started to be deployed in many important industrial applications stimulating fundamental theoretical work and development of experimental techniques. Here, we have studied local structure of supercritical matter by calculating static structure factor, mean force potential, self-diffusion, first coordination shell number and pair distribution function within very wide temperature range"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.7389","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":""},"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":"1405.7389","created_at":"2026-05-18T02:50:51.340585+00:00"},{"alias_kind":"arxiv_version","alias_value":"1405.7389v1","created_at":"2026-05-18T02:50:51.340585+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.7389","created_at":"2026-05-18T02:50:51.340585+00:00"},{"alias_kind":"pith_short_12","alias_value":"NKUNMOBBX3PW","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_16","alias_value":"NKUNMOBBX3PWLD6P","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_8","alias_value":"NKUNMOBB","created_at":"2026-05-18T12:28:41.024544+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/NKUNMOBBX3PWLD6PN4KOOPT6TB","json":"https://pith.science/pith/NKUNMOBBX3PWLD6PN4KOOPT6TB.json","graph_json":"https://pith.science/api/pith-number/NKUNMOBBX3PWLD6PN4KOOPT6TB/graph.json","events_json":"https://pith.science/api/pith-number/NKUNMOBBX3PWLD6PN4KOOPT6TB/events.json","paper":"https://pith.science/paper/NKUNMOBB"},"agent_actions":{"view_html":"https://pith.science/pith/NKUNMOBBX3PWLD6PN4KOOPT6TB","download_json":"https://pith.science/pith/NKUNMOBBX3PWLD6PN4KOOPT6TB.json","view_paper":"https://pith.science/paper/NKUNMOBB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1405.7389&json=true","fetch_graph":"https://pith.science/api/pith-number/NKUNMOBBX3PWLD6PN4KOOPT6TB/graph.json","fetch_events":"https://pith.science/api/pith-number/NKUNMOBBX3PWLD6PN4KOOPT6TB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NKUNMOBBX3PWLD6PN4KOOPT6TB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NKUNMOBBX3PWLD6PN4KOOPT6TB/action/storage_attestation","attest_author":"https://pith.science/pith/NKUNMOBBX3PWLD6PN4KOOPT6TB/action/author_attestation","sign_citation":"https://pith.science/pith/NKUNMOBBX3PWLD6PN4KOOPT6TB/action/citation_signature","submit_replication":"https://pith.science/pith/NKUNMOBBX3PWLD6PN4KOOPT6TB/action/replication_record"}},"created_at":"2026-05-18T02:50:51.340585+00:00","updated_at":"2026-05-18T02:50:51.340585+00:00"}