{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:CPOBLXMB3FKAX5I7IZLTAJDIYO","short_pith_number":"pith:CPOBLXMB","schema_version":"1.0","canonical_sha256":"13dc15dd81d9540bf51f4657302468c3ba80ff8f24ce972d24601273cb6cb15d","source":{"kind":"arxiv","id":"1812.08235","version":2},"attestation_state":"computed","paper":{"title":"Chiral crossover in QCD at zero and non-zero chemical potentials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Bazavov, Anirban Lahiri, C. Schmidt, E. Laermann, F. Karsch, H. Ohno, H. Sandmeyer, H.-T. Ding, N. Karthik, O. Kaczmarek, P. Hegde, P. Petreczky, P. Steinbrecher, R. Larsen, S. Sharma, S.-T. Li, Swagato Mukherjee","submitted_at":"2018-12-19T20:47:32Z","abstract_excerpt":"We present results for pseudo-critical temperatures of QCD chiral crossovers at zero and non-zero values of baryon ($B$), strangeness ($S$), electric charge ($Q$), and isospin ($I$) chemical potentials $\\mu_{X=B,Q,S,I}$. The results were obtained using lattice QCD calculations carried out with two degenerate up and down dynamical quarks and a dynamical strange quark, with quark masses corresponding to physical values of pion and kaon masses in the continuum limit. By parameterizing pseudo-critical temperatures as $ T_c(\\mu_X) = T_c(0) \\left[ 1 -\\kappa_2^{X}(\\mu_{X}/T_c(0))^2 -\\kappa_4^{X}(\\mu_"},"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":"1812.08235","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-12-19T20:47:32Z","cross_cats_sorted":["hep-ph","hep-th","nucl-ex","nucl-th"],"title_canon_sha256":"c5533e848d7543c878b7270b2549fe740250278fd1641d9a8a8f0c8d5043530e","abstract_canon_sha256":"7f677a4ea90c182dbad88cd9cff8bd8c265d8fb0b28a5e97a05a684953c93d8f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:26:38.011927Z","signature_b64":"i9+eROvha8U7zfcyZyrVPcauvrMLnr0c099ftD0rrQHpmNr0FTRXW7xnWHbtRimXl1IlREZzR4edZmYzrskGCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"13dc15dd81d9540bf51f4657302468c3ba80ff8f24ce972d24601273cb6cb15d","last_reissued_at":"2026-07-05T01:26:38.011371Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:26:38.011371Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chiral crossover in QCD at zero and non-zero chemical potentials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Bazavov, Anirban Lahiri, C. Schmidt, E. Laermann, F. Karsch, H. Ohno, H. Sandmeyer, H.-T. Ding, N. Karthik, O. Kaczmarek, P. Hegde, P. Petreczky, P. Steinbrecher, R. Larsen, S. Sharma, S.-T. Li, Swagato Mukherjee","submitted_at":"2018-12-19T20:47:32Z","abstract_excerpt":"We present results for pseudo-critical temperatures of QCD chiral crossovers at zero and non-zero values of baryon ($B$), strangeness ($S$), electric charge ($Q$), and isospin ($I$) chemical potentials $\\mu_{X=B,Q,S,I}$. The results were obtained using lattice QCD calculations carried out with two degenerate up and down dynamical quarks and a dynamical strange quark, with quark masses corresponding to physical values of pion and kaon masses in the continuum limit. By parameterizing pseudo-critical temperatures as $ T_c(\\mu_X) = T_c(0) \\left[ 1 -\\kappa_2^{X}(\\mu_{X}/T_c(0))^2 -\\kappa_4^{X}(\\mu_"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.08235","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1812.08235/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":"1812.08235","created_at":"2026-07-05T01:26:38.011444+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.08235v2","created_at":"2026-07-05T01:26:38.011444+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.08235","created_at":"2026-07-05T01:26:38.011444+00:00"},{"alias_kind":"pith_short_12","alias_value":"CPOBLXMB3FKA","created_at":"2026-07-05T01:26:38.011444+00:00"},{"alias_kind":"pith_short_16","alias_value":"CPOBLXMB3FKAX5I7","created_at":"2026-07-05T01:26:38.011444+00:00"},{"alias_kind":"pith_short_8","alias_value":"CPOBLXMB","created_at":"2026-07-05T01:26:38.011444+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":20,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07354","citing_title":"Fierz-complete four-quark interactions and the QCD phase diagram","ref_index":59,"is_internal_anchor":true},{"citing_arxiv_id":"2606.12619","citing_title":"Constraining the Low-$p_T$ $\\eta/\\pi^0$ Ratio for Direct-Photon Analyses with Blast-Wave Fits to $\\pi$, $K$, and $p$ Spectra","ref_index":4,"is_internal_anchor":false},{"citing_arxiv_id":"2606.12622","citing_title":"Analytic structure of the QCD phase diagram in the complex-temperature plane","ref_index":31,"is_internal_anchor":false},{"citing_arxiv_id":"2606.10356","citing_title":"Light and Strange Baryons in Medium","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2605.31280","citing_title":"Thermodynamics of the Isospectral family of holographic vector mesons","ref_index":53,"is_internal_anchor":false},{"citing_arxiv_id":"2605.30710","citing_title":"Canonical statistical hadronization with local baryon conservation for higher-order cumulants","ref_index":8,"is_internal_anchor":false},{"citing_arxiv_id":"2606.28086","citing_title":"The QCD phase diagram for three-flavor M\\\"obius domain-wall fermions","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2606.28282","citing_title":"QCD critical surface from constant entropy contours","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2606.30959","citing_title":"A multi-differential constraint map for quarkonium suppression mechanisms in high-multiplicity pp and pPb collisions","ref_index":6,"is_internal_anchor":false},{"citing_arxiv_id":"1907.08179","citing_title":"Strangeness neutrality and the QCD phase diagram","ref_index":9,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13934","citing_title":"Diquark Correlators and Phase Structure in the Quark-Meson-Diquark Model beyond Mean Field","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2510.06712","citing_title":"Dissecting the moat regime at low energies I: Renormalization and the phase structure","ref_index":10,"is_internal_anchor":false},{"citing_arxiv_id":"2510.22870","citing_title":"Mass and Decay-Constant Evolution of Heavy Quarkonia and $B_c$ States from Thermal QCD Sum Rules","ref_index":14,"is_internal_anchor":false},{"citing_arxiv_id":"2602.14811","citing_title":"RG-Invariant Symmetry Ratio for QCD: A Study of $U(1)_A$ and Chiral Symmetry Restoration","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2603.09977","citing_title":"Does hot QCD have a conformal manifold in the chiral limit?","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13934","citing_title":"Diquark Correlators and Phase Structure in the Quark-Meson-Diquark Model beyond Mean Field","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2604.03849","citing_title":"Two Lectures on the Phase Diagram of QCD","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2604.22514","citing_title":"Quark Number Susceptibilities and Conserved Charge Fluctuations in $(2+1)$-flavor QCD with M\\\"obius domain-wall fermions (MDWF)","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2604.22352","citing_title":"Four-dimensional QCD equation of state from a quasi-parton model with physics-informed neural networks","ref_index":17,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19649","citing_title":"Finite-density equation of state of hot QCD using the complex Langevin equation","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CPOBLXMB3FKAX5I7IZLTAJDIYO","json":"https://pith.science/pith/CPOBLXMB3FKAX5I7IZLTAJDIYO.json","graph_json":"https://pith.science/api/pith-number/CPOBLXMB3FKAX5I7IZLTAJDIYO/graph.json","events_json":"https://pith.science/api/pith-number/CPOBLXMB3FKAX5I7IZLTAJDIYO/events.json","paper":"https://pith.science/paper/CPOBLXMB"},"agent_actions":{"view_html":"https://pith.science/pith/CPOBLXMB3FKAX5I7IZLTAJDIYO","download_json":"https://pith.science/pith/CPOBLXMB3FKAX5I7IZLTAJDIYO.json","view_paper":"https://pith.science/paper/CPOBLXMB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.08235&json=true","fetch_graph":"https://pith.science/api/pith-number/CPOBLXMB3FKAX5I7IZLTAJDIYO/graph.json","fetch_events":"https://pith.science/api/pith-number/CPOBLXMB3FKAX5I7IZLTAJDIYO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CPOBLXMB3FKAX5I7IZLTAJDIYO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CPOBLXMB3FKAX5I7IZLTAJDIYO/action/storage_attestation","attest_author":"https://pith.science/pith/CPOBLXMB3FKAX5I7IZLTAJDIYO/action/author_attestation","sign_citation":"https://pith.science/pith/CPOBLXMB3FKAX5I7IZLTAJDIYO/action/citation_signature","submit_replication":"https://pith.science/pith/CPOBLXMB3FKAX5I7IZLTAJDIYO/action/replication_record"}},"created_at":"2026-07-05T01:26:38.011444+00:00","updated_at":"2026-07-05T01:26:38.011444+00:00"}