{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:WQZ5L2WZYBYZJEBXZIEXQXYRG3","short_pith_number":"pith:WQZ5L2WZ","schema_version":"1.0","canonical_sha256":"b433d5ead9c071949037ca09785f1136cba9ef30221a941e6e1a8f8a06fa1a13","source":{"kind":"arxiv","id":"1503.05211","version":1},"attestation_state":"computed","paper":{"title":"The critical end point through observables","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. Kozlov","submitted_at":"2015-03-17T20:22:10Z","abstract_excerpt":"We develop the model of the critical phenomena of strongly interacting matter at high temperatures and baryon densities. The dual Yang-Mills theory with scalar degrees of freedom (the dilatons) is used. The dilatons are the consequence of a spontaneous breaking of a scale symmetry. The phase transitions are considered in systems where the field conjugate to the order parameter has the critical end mode. The critical end point (CEP) is a distinct singular feature existence of which is dictated by the chiral dynamics. The physical realization of CEP is via the influence quantum fluctuations of t"},"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":"1503.05211","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-03-17T20:22:10Z","cross_cats_sorted":[],"title_canon_sha256":"6dde0c330d94d5fc411438ab4ac526ba33842334940ac5d91a6f4249ea006263","abstract_canon_sha256":"29edb8eed95e83ab0b031acb13325fc4f6a6270cd425337e5d1730eeb14db847"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:46.816902Z","signature_b64":"c+3WpLV2r3SscIEs5fZroeGUX9nx/6dT2xI1ON1inucZXZtJHC3zBiUXTcMtTDhAVUeIjCsrqJHlwFzaPSvVBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b433d5ead9c071949037ca09785f1136cba9ef30221a941e6e1a8f8a06fa1a13","last_reissued_at":"2026-05-18T01:20:46.816377Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:46.816377Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The critical end point through observables","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. Kozlov","submitted_at":"2015-03-17T20:22:10Z","abstract_excerpt":"We develop the model of the critical phenomena of strongly interacting matter at high temperatures and baryon densities. The dual Yang-Mills theory with scalar degrees of freedom (the dilatons) is used. The dilatons are the consequence of a spontaneous breaking of a scale symmetry. The phase transitions are considered in systems where the field conjugate to the order parameter has the critical end mode. The critical end point (CEP) is a distinct singular feature existence of which is dictated by the chiral dynamics. The physical realization of CEP is via the influence quantum fluctuations of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.05211","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":"1503.05211","created_at":"2026-05-18T01:20:46.816457+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.05211v1","created_at":"2026-05-18T01:20:46.816457+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.05211","created_at":"2026-05-18T01:20:46.816457+00:00"},{"alias_kind":"pith_short_12","alias_value":"WQZ5L2WZYBYZ","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_16","alias_value":"WQZ5L2WZYBYZJEBX","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_8","alias_value":"WQZ5L2WZ","created_at":"2026-05-18T12:29:47.479230+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/WQZ5L2WZYBYZJEBXZIEXQXYRG3","json":"https://pith.science/pith/WQZ5L2WZYBYZJEBXZIEXQXYRG3.json","graph_json":"https://pith.science/api/pith-number/WQZ5L2WZYBYZJEBXZIEXQXYRG3/graph.json","events_json":"https://pith.science/api/pith-number/WQZ5L2WZYBYZJEBXZIEXQXYRG3/events.json","paper":"https://pith.science/paper/WQZ5L2WZ"},"agent_actions":{"view_html":"https://pith.science/pith/WQZ5L2WZYBYZJEBXZIEXQXYRG3","download_json":"https://pith.science/pith/WQZ5L2WZYBYZJEBXZIEXQXYRG3.json","view_paper":"https://pith.science/paper/WQZ5L2WZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.05211&json=true","fetch_graph":"https://pith.science/api/pith-number/WQZ5L2WZYBYZJEBXZIEXQXYRG3/graph.json","fetch_events":"https://pith.science/api/pith-number/WQZ5L2WZYBYZJEBXZIEXQXYRG3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WQZ5L2WZYBYZJEBXZIEXQXYRG3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WQZ5L2WZYBYZJEBXZIEXQXYRG3/action/storage_attestation","attest_author":"https://pith.science/pith/WQZ5L2WZYBYZJEBXZIEXQXYRG3/action/author_attestation","sign_citation":"https://pith.science/pith/WQZ5L2WZYBYZJEBXZIEXQXYRG3/action/citation_signature","submit_replication":"https://pith.science/pith/WQZ5L2WZYBYZJEBXZIEXQXYRG3/action/replication_record"}},"created_at":"2026-05-18T01:20:46.816457+00:00","updated_at":"2026-05-18T01:20:46.816457+00:00"}