{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:VM2BNBM5NFTL2JZT2T3EGZGOL2","short_pith_number":"pith:VM2BNBM5","schema_version":"1.0","canonical_sha256":"ab3416859d6966bd2733d4f64364ce5eb539b529b6f4909c834b2b7e0b1a19ca","source":{"kind":"arxiv","id":"1610.08748","version":2},"attestation_state":"computed","paper":{"title":"Fluctuation-induced modifications of the phase structure in (2+1)-flavor QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Bernd-Jochen Schaefer, Fabian Rennecke","submitted_at":"2016-10-27T12:31:16Z","abstract_excerpt":"The low-energy sector of QCD with $N_f = 2\\!+\\!1$ dynamical quark flavors at non-vanishing chemical potential and temperature is studied with a non-perturbative functional renormalization group method. The analysis is performed in different truncations in order to explore fluctuation-induced modifications of the quark-meson correlations as well as quark and meson propagators on the chiral phase transition of QCD. Depending on the chosen truncation significant quantitative implications on the phase transition are found. In the chirally symmetric phase, the quark flavor composition of the pseudo"},"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":"1610.08748","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-27T12:31:16Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"475412ecfee83403f27ebaa00843f2bb2d5cae00d9b06e37b565203c8dc5fa09","abstract_canon_sha256":"1711c107d08c189f54bc54810ecb115b5b324ef2e597c0612ea7e789b492fbaf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:39:39.807909Z","signature_b64":"rbHwpvAEOjph+Yab/aq7yykgkUrPkhl/7z+2SzjaR9Cv60CpE3XTtXV5mtMA2ocCj+nwusl55S7/WB6I8qnEAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ab3416859d6966bd2733d4f64364ce5eb539b529b6f4909c834b2b7e0b1a19ca","last_reissued_at":"2026-05-18T00:39:39.807289Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:39:39.807289Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fluctuation-induced modifications of the phase structure in (2+1)-flavor QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Bernd-Jochen Schaefer, Fabian Rennecke","submitted_at":"2016-10-27T12:31:16Z","abstract_excerpt":"The low-energy sector of QCD with $N_f = 2\\!+\\!1$ dynamical quark flavors at non-vanishing chemical potential and temperature is studied with a non-perturbative functional renormalization group method. The analysis is performed in different truncations in order to explore fluctuation-induced modifications of the quark-meson correlations as well as quark and meson propagators on the chiral phase transition of QCD. Depending on the chosen truncation significant quantitative implications on the phase transition are found. In the chirally symmetric phase, the quark flavor composition of the pseudo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.08748","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":"1610.08748","created_at":"2026-05-18T00:39:39.807404+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.08748v2","created_at":"2026-05-18T00:39:39.807404+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.08748","created_at":"2026-05-18T00:39:39.807404+00:00"},{"alias_kind":"pith_short_12","alias_value":"VM2BNBM5NFTL","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_16","alias_value":"VM2BNBM5NFTL2JZT","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_8","alias_value":"VM2BNBM5","created_at":"2026-05-18T12:30:48.956258+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"1907.08179","citing_title":"Strangeness neutrality and the QCD phase diagram","ref_index":21,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13934","citing_title":"Diquark Correlators and Phase Structure in the Quark-Meson-Diquark Model beyond Mean Field","ref_index":60,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13934","citing_title":"Diquark Correlators and Phase Structure in the Quark-Meson-Diquark Model beyond Mean Field","ref_index":60,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VM2BNBM5NFTL2JZT2T3EGZGOL2","json":"https://pith.science/pith/VM2BNBM5NFTL2JZT2T3EGZGOL2.json","graph_json":"https://pith.science/api/pith-number/VM2BNBM5NFTL2JZT2T3EGZGOL2/graph.json","events_json":"https://pith.science/api/pith-number/VM2BNBM5NFTL2JZT2T3EGZGOL2/events.json","paper":"https://pith.science/paper/VM2BNBM5"},"agent_actions":{"view_html":"https://pith.science/pith/VM2BNBM5NFTL2JZT2T3EGZGOL2","download_json":"https://pith.science/pith/VM2BNBM5NFTL2JZT2T3EGZGOL2.json","view_paper":"https://pith.science/paper/VM2BNBM5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.08748&json=true","fetch_graph":"https://pith.science/api/pith-number/VM2BNBM5NFTL2JZT2T3EGZGOL2/graph.json","fetch_events":"https://pith.science/api/pith-number/VM2BNBM5NFTL2JZT2T3EGZGOL2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VM2BNBM5NFTL2JZT2T3EGZGOL2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VM2BNBM5NFTL2JZT2T3EGZGOL2/action/storage_attestation","attest_author":"https://pith.science/pith/VM2BNBM5NFTL2JZT2T3EGZGOL2/action/author_attestation","sign_citation":"https://pith.science/pith/VM2BNBM5NFTL2JZT2T3EGZGOL2/action/citation_signature","submit_replication":"https://pith.science/pith/VM2BNBM5NFTL2JZT2T3EGZGOL2/action/replication_record"}},"created_at":"2026-05-18T00:39:39.807404+00:00","updated_at":"2026-05-18T00:39:39.807404+00:00"}