{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:KAIX7WI7LSRKJJJIFJBW225GOX","short_pith_number":"pith:KAIX7WI7","schema_version":"1.0","canonical_sha256":"50117fd91f5ca2a4a5282a436d6ba675c209e49974d6a17bcb7167c03b476636","source":{"kind":"arxiv","id":"1302.2835","version":2},"attestation_state":"computed","paper":{"title":"Non-congruence of the nuclear liquid-gas and deconfinement phase transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE","astro-ph.SR"],"primary_cat":"nucl-th","authors_text":"Igor Iosilevskiy, Matthias Hempel, Stefan Schramm, Veronica Dexheimer","submitted_at":"2013-02-12T16:06:53Z","abstract_excerpt":"First order phase transitions (PTs) with more than one globally conserved charge, so-called non-congruent PTs, have characteristic differences compared to congruent PTs (e.g., dimensionality of phase diagrams, location and properties of critical points and endpoints). In the present article we investigate the non-congruence of the nuclear liquid-gas PT at sub-saturation densities and the deconfinement PT at high densities and/or temperatures in Coulomb-less models, relevant for heavy-ion collisions and neutron stars. For the first PT, we use the FSUgold relativistic mean-field model and for th"},"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":"1302.2835","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-02-12T16:06:53Z","cross_cats_sorted":["astro-ph.HE","astro-ph.SR"],"title_canon_sha256":"f93afd3ee50dd9552aa46a2703c543805b4862f398a583154205694fc0bc2584","abstract_canon_sha256":"7db15db60dfb2e5dc63c4bb80533af98f71e3fce69826173ba6b606bceac4aa8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:03:55.895122Z","signature_b64":"Lx4D+MC3+05yfiVOHaW59unw1muiY1DcJc8t3bmvYOZHjV+MIb2n6PRrCIzrq/pKpSlnhqQGAvOa+ulMVm3sCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"50117fd91f5ca2a4a5282a436d6ba675c209e49974d6a17bcb7167c03b476636","last_reissued_at":"2026-05-18T02:03:55.894369Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:03:55.894369Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-congruence of the nuclear liquid-gas and deconfinement phase transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE","astro-ph.SR"],"primary_cat":"nucl-th","authors_text":"Igor Iosilevskiy, Matthias Hempel, Stefan Schramm, Veronica Dexheimer","submitted_at":"2013-02-12T16:06:53Z","abstract_excerpt":"First order phase transitions (PTs) with more than one globally conserved charge, so-called non-congruent PTs, have characteristic differences compared to congruent PTs (e.g., dimensionality of phase diagrams, location and properties of critical points and endpoints). In the present article we investigate the non-congruence of the nuclear liquid-gas PT at sub-saturation densities and the deconfinement PT at high densities and/or temperatures in Coulomb-less models, relevant for heavy-ion collisions and neutron stars. For the first PT, we use the FSUgold relativistic mean-field model and for th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.2835","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":"1302.2835","created_at":"2026-05-18T02:03:55.894488+00:00"},{"alias_kind":"arxiv_version","alias_value":"1302.2835v2","created_at":"2026-05-18T02:03:55.894488+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.2835","created_at":"2026-05-18T02:03:55.894488+00:00"},{"alias_kind":"pith_short_12","alias_value":"KAIX7WI7LSRK","created_at":"2026-05-18T12:27:49.015174+00:00"},{"alias_kind":"pith_short_16","alias_value":"KAIX7WI7LSRKJJJI","created_at":"2026-05-18T12:27:49.015174+00:00"},{"alias_kind":"pith_short_8","alias_value":"KAIX7WI7","created_at":"2026-05-18T12:27:49.015174+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/KAIX7WI7LSRKJJJIFJBW225GOX","json":"https://pith.science/pith/KAIX7WI7LSRKJJJIFJBW225GOX.json","graph_json":"https://pith.science/api/pith-number/KAIX7WI7LSRKJJJIFJBW225GOX/graph.json","events_json":"https://pith.science/api/pith-number/KAIX7WI7LSRKJJJIFJBW225GOX/events.json","paper":"https://pith.science/paper/KAIX7WI7"},"agent_actions":{"view_html":"https://pith.science/pith/KAIX7WI7LSRKJJJIFJBW225GOX","download_json":"https://pith.science/pith/KAIX7WI7LSRKJJJIFJBW225GOX.json","view_paper":"https://pith.science/paper/KAIX7WI7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1302.2835&json=true","fetch_graph":"https://pith.science/api/pith-number/KAIX7WI7LSRKJJJIFJBW225GOX/graph.json","fetch_events":"https://pith.science/api/pith-number/KAIX7WI7LSRKJJJIFJBW225GOX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KAIX7WI7LSRKJJJIFJBW225GOX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KAIX7WI7LSRKJJJIFJBW225GOX/action/storage_attestation","attest_author":"https://pith.science/pith/KAIX7WI7LSRKJJJIFJBW225GOX/action/author_attestation","sign_citation":"https://pith.science/pith/KAIX7WI7LSRKJJJIFJBW225GOX/action/citation_signature","submit_replication":"https://pith.science/pith/KAIX7WI7LSRKJJJIFJBW225GOX/action/replication_record"}},"created_at":"2026-05-18T02:03:55.894488+00:00","updated_at":"2026-05-18T02:03:55.894488+00:00"}