{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:5Q5BBVXKTSWN5EZRXSN7B67D3F","short_pith_number":"pith:5Q5BBVXK","schema_version":"1.0","canonical_sha256":"ec3a10d6ea9cacde9331bc9bf0fbe3d9520354cb305bdb59d0b1d88e922b9511","source":{"kind":"arxiv","id":"1703.05947","version":1},"attestation_state":"computed","paper":{"title":"Baryon number fluctuations in chiral effective models and their phenomenological implications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Bengt Friman, Gabor Almasi, Krzysztof Redlich","submitted_at":"2017-03-17T10:05:50Z","abstract_excerpt":"We study the critical properties of net-baryon-number fluctuations at the chiral restoration transition in a medium at finite temperature and net baryon density. The chiral dynamics of quantum chromodynamics (QCD) is modeled by the Polykov-loop extended Quark-Meson Lagrangian, that includes the coupling of quarks to vector meson and temporal gauge fields. The Functional Renormalization Group is employed to properly account for the $O(4)$ criticality at the phase boundary. We focus on the properties and systematics of ratios of the net-baryon-number cumulants $\\chi_B^n$, for ${1\\leq n\\leq 6}$, "},"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":"1703.05947","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-03-17T10:05:50Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"c190abc5fb1c1103c880f44cc6fc3e1829b8e5a8f87b4c225d478e0cbad187d0","abstract_canon_sha256":"697438c9b97c0edce25c07af90382f7225494622262e417ede092fbfae4cfea3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:56.611633Z","signature_b64":"7e0miJ+tIL23w3Q3ILQtYjQ4x5XtlU8SpTv6HHEZtyqiRMEHU4ksbaSorO9mU5eRZIgR+YrMRjgxHIa4b73NDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ec3a10d6ea9cacde9331bc9bf0fbe3d9520354cb305bdb59d0b1d88e922b9511","last_reissued_at":"2026-05-18T00:38:56.610997Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:56.610997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryon number fluctuations in chiral effective models and their phenomenological implications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Bengt Friman, Gabor Almasi, Krzysztof Redlich","submitted_at":"2017-03-17T10:05:50Z","abstract_excerpt":"We study the critical properties of net-baryon-number fluctuations at the chiral restoration transition in a medium at finite temperature and net baryon density. The chiral dynamics of quantum chromodynamics (QCD) is modeled by the Polykov-loop extended Quark-Meson Lagrangian, that includes the coupling of quarks to vector meson and temporal gauge fields. The Functional Renormalization Group is employed to properly account for the $O(4)$ criticality at the phase boundary. We focus on the properties and systematics of ratios of the net-baryon-number cumulants $\\chi_B^n$, for ${1\\leq n\\leq 6}$, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.05947","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":"1703.05947","created_at":"2026-05-18T00:38:56.611070+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.05947v1","created_at":"2026-05-18T00:38:56.611070+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.05947","created_at":"2026-05-18T00:38:56.611070+00:00"},{"alias_kind":"pith_short_12","alias_value":"5Q5BBVXKTSWN","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_16","alias_value":"5Q5BBVXKTSWN5EZR","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_8","alias_value":"5Q5BBVXK","created_at":"2026-05-18T12:31:00.734936+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/5Q5BBVXKTSWN5EZRXSN7B67D3F","json":"https://pith.science/pith/5Q5BBVXKTSWN5EZRXSN7B67D3F.json","graph_json":"https://pith.science/api/pith-number/5Q5BBVXKTSWN5EZRXSN7B67D3F/graph.json","events_json":"https://pith.science/api/pith-number/5Q5BBVXKTSWN5EZRXSN7B67D3F/events.json","paper":"https://pith.science/paper/5Q5BBVXK"},"agent_actions":{"view_html":"https://pith.science/pith/5Q5BBVXKTSWN5EZRXSN7B67D3F","download_json":"https://pith.science/pith/5Q5BBVXKTSWN5EZRXSN7B67D3F.json","view_paper":"https://pith.science/paper/5Q5BBVXK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.05947&json=true","fetch_graph":"https://pith.science/api/pith-number/5Q5BBVXKTSWN5EZRXSN7B67D3F/graph.json","fetch_events":"https://pith.science/api/pith-number/5Q5BBVXKTSWN5EZRXSN7B67D3F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5Q5BBVXKTSWN5EZRXSN7B67D3F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5Q5BBVXKTSWN5EZRXSN7B67D3F/action/storage_attestation","attest_author":"https://pith.science/pith/5Q5BBVXKTSWN5EZRXSN7B67D3F/action/author_attestation","sign_citation":"https://pith.science/pith/5Q5BBVXKTSWN5EZRXSN7B67D3F/action/citation_signature","submit_replication":"https://pith.science/pith/5Q5BBVXKTSWN5EZRXSN7B67D3F/action/replication_record"}},"created_at":"2026-05-18T00:38:56.611070+00:00","updated_at":"2026-05-18T00:38:56.611070+00:00"}