{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:6YNGLPKHPNSQPQZWDDIKPFPOOC","short_pith_number":"pith:6YNGLPKH","schema_version":"1.0","canonical_sha256":"f61a65bd477b6507c33618d0a795ee70be9221aa7727f934f1b98244d79054c5","source":{"kind":"arxiv","id":"1111.1710","version":2},"attestation_state":"computed","paper":{"title":"The chiral and deconfinement aspects of the QCD transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Bazavov, C. DeTar, C. Schmidt, D. Toussaint, E. Laermann, F. Karsch, H.-T. Ding, L. Levkova, M. Cheng, P. Hegde, P. Petreczky, P. Vranas, R. A. Soltz, R. Gupta, R. Sugar, S. Mukherjee, Steven Gottlieb, T. Bhattacharya, U. M. Heller, W. Soeldner, W. Unger","submitted_at":"2011-11-07T20:57:56Z","abstract_excerpt":"We present results on the chiral and deconfinement properties of the QCD transition at finite temperature. Calculations are performed with 2+1 flavors of quarks using the p4, asqtad and HISQ/tree actions. Lattices with temporal extent N_tau=6, 8 and 12 are used to understand and control discretization errors and to reliably extrapolate estimates obtained at finite lattice spacings to the continuum limit. The chiral transition temperature is defined in terms of the phase transition in a theory with two massless flavors and analyzed using O(N) scaling fits to the chiral condensate and susceptibi"},"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":"1111.1710","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2011-11-07T20:57:56Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"40a17e6ab1d86687dbd70688d2585c3b9c018ff3e768a2e1890e985d4160eaaa","abstract_canon_sha256":"03b2124a1a734933e4ef38decc4cc30ca28c9362dbff5e96dd364ffd755ce1aa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:44.262094Z","signature_b64":"foTlFd9q5O4S3mOIxo3xVCZ4lQ7q5xSaxR0axBlHVR4JWfXwPJ+KHP0oOY4gTRTndeh4/AZhWvR8VDYG6jOwBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f61a65bd477b6507c33618d0a795ee70be9221aa7727f934f1b98244d79054c5","last_reissued_at":"2026-05-18T01:59:44.261210Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:44.261210Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The chiral and deconfinement aspects of the QCD transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"A. Bazavov, C. DeTar, C. Schmidt, D. Toussaint, E. Laermann, F. Karsch, H.-T. Ding, L. Levkova, M. Cheng, P. Hegde, P. Petreczky, P. Vranas, R. A. Soltz, R. Gupta, R. Sugar, S. Mukherjee, Steven Gottlieb, T. Bhattacharya, U. M. Heller, W. Soeldner, W. Unger","submitted_at":"2011-11-07T20:57:56Z","abstract_excerpt":"We present results on the chiral and deconfinement properties of the QCD transition at finite temperature. Calculations are performed with 2+1 flavors of quarks using the p4, asqtad and HISQ/tree actions. Lattices with temporal extent N_tau=6, 8 and 12 are used to understand and control discretization errors and to reliably extrapolate estimates obtained at finite lattice spacings to the continuum limit. The chiral transition temperature is defined in terms of the phase transition in a theory with two massless flavors and analyzed using O(N) scaling fits to the chiral condensate and susceptibi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.1710","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":"1111.1710","created_at":"2026-05-18T01:59:44.261371+00:00"},{"alias_kind":"arxiv_version","alias_value":"1111.1710v2","created_at":"2026-05-18T01:59:44.261371+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.1710","created_at":"2026-05-18T01:59:44.261371+00:00"},{"alias_kind":"pith_short_12","alias_value":"6YNGLPKHPNSQ","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_16","alias_value":"6YNGLPKHPNSQPQZW","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_8","alias_value":"6YNGLPKH","created_at":"2026-05-18T12:26:22.705136+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":12,"internal_anchor_count":7,"sample":[{"citing_arxiv_id":"1907.03032","citing_title":"The role of the local conservation laws in fluctuations of conserved charges","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"2601.18354","citing_title":"Chiral Properties of $(2\\!+\\!1)$-Flavor QCD in Magnetic Fields at Zero Temperature","ref_index":97,"is_internal_anchor":true},{"citing_arxiv_id":"2509.14323","citing_title":"High-Quality Axion Dark Matter at Gravitational Wave Interferometers","ref_index":95,"is_internal_anchor":true},{"citing_arxiv_id":"2509.24316","citing_title":"Energy loss of heavy-flavor quarks in color string medium","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"2511.19255","citing_title":"Magnetic susceptibility of a hot hadronic medium and quark degrees of freedom near the QCD cross-over point","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2512.02635","citing_title":"Unified Functional-Holographic Theory of the QCD Critical End Point","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"2003.01100","citing_title":"The landscape of QCD axion models","ref_index":172,"is_internal_anchor":true},{"citing_arxiv_id":"2604.03849","citing_title":"Two Lectures on the Phase Diagram of QCD","ref_index":21,"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":17,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04558","citing_title":"Effects of event-by-event hydrodynamic fluctuations on bottomonium dynamics in Pb--Pb collisions at $\\sqrt{s_{NN}} = 5.02$ TeV","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2604.09198","citing_title":"Unified Extraction of In-Medium Heavy Quark Potentials from RHIC to LHC Energies via Deep Learning","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15737","citing_title":"Bayesian inference constraints on jet quenching across centrality, beam energy, and observable classes in LHC heavy-ion collisions","ref_index":99,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6YNGLPKHPNSQPQZWDDIKPFPOOC","json":"https://pith.science/pith/6YNGLPKHPNSQPQZWDDIKPFPOOC.json","graph_json":"https://pith.science/api/pith-number/6YNGLPKHPNSQPQZWDDIKPFPOOC/graph.json","events_json":"https://pith.science/api/pith-number/6YNGLPKHPNSQPQZWDDIKPFPOOC/events.json","paper":"https://pith.science/paper/6YNGLPKH"},"agent_actions":{"view_html":"https://pith.science/pith/6YNGLPKHPNSQPQZWDDIKPFPOOC","download_json":"https://pith.science/pith/6YNGLPKHPNSQPQZWDDIKPFPOOC.json","view_paper":"https://pith.science/paper/6YNGLPKH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1111.1710&json=true","fetch_graph":"https://pith.science/api/pith-number/6YNGLPKHPNSQPQZWDDIKPFPOOC/graph.json","fetch_events":"https://pith.science/api/pith-number/6YNGLPKHPNSQPQZWDDIKPFPOOC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6YNGLPKHPNSQPQZWDDIKPFPOOC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6YNGLPKHPNSQPQZWDDIKPFPOOC/action/storage_attestation","attest_author":"https://pith.science/pith/6YNGLPKHPNSQPQZWDDIKPFPOOC/action/author_attestation","sign_citation":"https://pith.science/pith/6YNGLPKHPNSQPQZWDDIKPFPOOC/action/citation_signature","submit_replication":"https://pith.science/pith/6YNGLPKHPNSQPQZWDDIKPFPOOC/action/replication_record"}},"created_at":"2026-05-18T01:59:44.261371+00:00","updated_at":"2026-05-18T01:59:44.261371+00:00"}