{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:C2TRWWJNSEMOCBQ6V4ISXVSHN5","short_pith_number":"pith:C2TRWWJN","schema_version":"1.0","canonical_sha256":"16a71b592d9118e1061eaf112bd6476f6724dc2105e817057677ecfa5bc3b65e","source":{"kind":"arxiv","id":"1811.05081","version":1},"attestation_state":"computed","paper":{"title":"Transits of the QCD Critical Point","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"nucl-th","authors_text":"Derek Teaney, Fanglida Yan, Yi Yin, Yukinao Akamatsu","submitted_at":"2018-11-13T03:02:27Z","abstract_excerpt":"We analyze the evolution of hydrodynamic fluctuations in a heavy ion collision as the system passes close to the QCD critical point. We introduce two small dimensionless parameters $\\lambda$ and $\\Delta_s$ to characterize the evolution. $\\lambda$ compares the microscopic relaxation time (away from the critical point) to the expansion rate $\\lambda \\equiv \\tau_0/\\tau_Q$, and $\\Delta_s$ compares the baryon to entropy ratio, $n/s$, to its critical value, $\\Delta_s\\equiv (n/s - n_c/s_c)/(n_c/s_c)$. We determine how the evolution of critical hydrodynamic fluctuations depends parametrically on $\\lam"},"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":"1811.05081","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2018-11-13T03:02:27Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"90e1022e33bddda1887bcd8c9af982b834639c746903dfcd025ff889346a3edd","abstract_canon_sha256":"572e9466470c48278e29d98ab316a6eb207f2378412141a13d93c949410eb6a7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:10:32.466616Z","signature_b64":"KlfJ1JvtRYHnz05fa311YFOP1+90sF+PkLlqotcfQfdPKTs2+NcPJz3Fy+SUMR+o0mg9LSqLOrlCpDXQbFMzAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"16a71b592d9118e1061eaf112bd6476f6724dc2105e817057677ecfa5bc3b65e","last_reissued_at":"2026-07-05T00:10:32.466206Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:10:32.466206Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transits of the QCD Critical Point","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"nucl-th","authors_text":"Derek Teaney, Fanglida Yan, Yi Yin, Yukinao Akamatsu","submitted_at":"2018-11-13T03:02:27Z","abstract_excerpt":"We analyze the evolution of hydrodynamic fluctuations in a heavy ion collision as the system passes close to the QCD critical point. We introduce two small dimensionless parameters $\\lambda$ and $\\Delta_s$ to characterize the evolution. $\\lambda$ compares the microscopic relaxation time (away from the critical point) to the expansion rate $\\lambda \\equiv \\tau_0/\\tau_Q$, and $\\Delta_s$ compares the baryon to entropy ratio, $n/s$, to its critical value, $\\Delta_s\\equiv (n/s - n_c/s_c)/(n_c/s_c)$. We determine how the evolution of critical hydrodynamic fluctuations depends parametrically on $\\lam"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.05081","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/1811.05081/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":"1811.05081","created_at":"2026-07-05T00:10:32.466262+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.05081v1","created_at":"2026-07-05T00:10:32.466262+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.05081","created_at":"2026-07-05T00:10:32.466262+00:00"},{"alias_kind":"pith_short_12","alias_value":"C2TRWWJNSEMO","created_at":"2026-07-05T00:10:32.466262+00:00"},{"alias_kind":"pith_short_16","alias_value":"C2TRWWJNSEMOCBQ6","created_at":"2026-07-05T00:10:32.466262+00:00"},{"alias_kind":"pith_short_8","alias_value":"C2TRWWJN","created_at":"2026-07-05T00:10:32.466262+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/C2TRWWJNSEMOCBQ6V4ISXVSHN5","json":"https://pith.science/pith/C2TRWWJNSEMOCBQ6V4ISXVSHN5.json","graph_json":"https://pith.science/api/pith-number/C2TRWWJNSEMOCBQ6V4ISXVSHN5/graph.json","events_json":"https://pith.science/api/pith-number/C2TRWWJNSEMOCBQ6V4ISXVSHN5/events.json","paper":"https://pith.science/paper/C2TRWWJN"},"agent_actions":{"view_html":"https://pith.science/pith/C2TRWWJNSEMOCBQ6V4ISXVSHN5","download_json":"https://pith.science/pith/C2TRWWJNSEMOCBQ6V4ISXVSHN5.json","view_paper":"https://pith.science/paper/C2TRWWJN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.05081&json=true","fetch_graph":"https://pith.science/api/pith-number/C2TRWWJNSEMOCBQ6V4ISXVSHN5/graph.json","fetch_events":"https://pith.science/api/pith-number/C2TRWWJNSEMOCBQ6V4ISXVSHN5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C2TRWWJNSEMOCBQ6V4ISXVSHN5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C2TRWWJNSEMOCBQ6V4ISXVSHN5/action/storage_attestation","attest_author":"https://pith.science/pith/C2TRWWJNSEMOCBQ6V4ISXVSHN5/action/author_attestation","sign_citation":"https://pith.science/pith/C2TRWWJNSEMOCBQ6V4ISXVSHN5/action/citation_signature","submit_replication":"https://pith.science/pith/C2TRWWJNSEMOCBQ6V4ISXVSHN5/action/replication_record"}},"created_at":"2026-07-05T00:10:32.466262+00:00","updated_at":"2026-07-05T00:10:32.466262+00:00"}