{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:IU4QUEI6XGHYP4XZUSHXHANY2F","short_pith_number":"pith:IU4QUEI6","schema_version":"1.0","canonical_sha256":"45390a111eb98f87f2f9a48f7381b8d16c31dded7f7c9f20aa4406cd11acd3cf","source":{"kind":"arxiv","id":"2009.14033","version":2},"attestation_state":"computed","paper":{"title":"Deconfinement critical point of lattice QCD with $N_{\\rm f}=2$ Wilson fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Alena Sch\\\"on, Alessandro Sciarra, Francesca Cuteri, Owe Philipsen","submitted_at":"2020-09-29T14:06:51Z","abstract_excerpt":"The ${\\rm SU}(3)$ pure gauge theory exhibits a first-order thermal deconfinement transition due to spontaneous breaking of its global $Z_3$ center symmetry. When heavy dynamical quarks are added, this symmetry is broken explicitly and the transition weakens with decreasing quark mass until it disappears at a critical point. We compute the critical hopping parameter and the associated pion mass for lattice QCD with $N_f=2$ degenerate standard Wilson fermions on $N_\\tau\\in\\{6,8,10\\}$ lattices, corresponding to lattice spacings $a=0.12\\, {\\rm fm}$, $a=0.09\\, {\\rm fm}$, $a=0.07\\, {\\rm fm}$, respec"},"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":"2009.14033","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2020-09-29T14:06:51Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"14701c2f894f0f5166cc4d5f4a0181f99bcd644603026ad7a16255d5e34e3988","abstract_canon_sha256":"88d0fb7303a92b133d1b3e5f86396412b0587154b9dea9a177adb0cd1ddefe2e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:08:50.596665Z","signature_b64":"HjdzAWZhKHH7FgVuo5Pp4Ov6lQFfLbsj04lnMHltVKIkCpVUo5h6kpKfXKUw+NzwOqL8CgY3US4OMY8hwnwkCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"45390a111eb98f87f2f9a48f7381b8d16c31dded7f7c9f20aa4406cd11acd3cf","last_reissued_at":"2026-07-05T02:08:50.596155Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:08:50.596155Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Deconfinement critical point of lattice QCD with $N_{\\rm f}=2$ Wilson fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Alena Sch\\\"on, Alessandro Sciarra, Francesca Cuteri, Owe Philipsen","submitted_at":"2020-09-29T14:06:51Z","abstract_excerpt":"The ${\\rm SU}(3)$ pure gauge theory exhibits a first-order thermal deconfinement transition due to spontaneous breaking of its global $Z_3$ center symmetry. When heavy dynamical quarks are added, this symmetry is broken explicitly and the transition weakens with decreasing quark mass until it disappears at a critical point. We compute the critical hopping parameter and the associated pion mass for lattice QCD with $N_f=2$ degenerate standard Wilson fermions on $N_\\tau\\in\\{6,8,10\\}$ lattices, corresponding to lattice spacings $a=0.12\\, {\\rm fm}$, $a=0.09\\, {\\rm fm}$, $a=0.07\\, {\\rm fm}$, respec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2009.14033","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/2009.14033/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":"2009.14033","created_at":"2026-07-05T02:08:50.596214+00:00"},{"alias_kind":"arxiv_version","alias_value":"2009.14033v2","created_at":"2026-07-05T02:08:50.596214+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2009.14033","created_at":"2026-07-05T02:08:50.596214+00:00"},{"alias_kind":"pith_short_12","alias_value":"IU4QUEI6XGHY","created_at":"2026-07-05T02:08:50.596214+00:00"},{"alias_kind":"pith_short_16","alias_value":"IU4QUEI6XGHYP4XZ","created_at":"2026-07-05T02:08:50.596214+00:00"},{"alias_kind":"pith_short_8","alias_value":"IU4QUEI6","created_at":"2026-07-05T02:08:50.596214+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.31492","citing_title":"Higher-order hopping-parameter expansion by human-AI collaboration","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2605.19964","citing_title":"Lee-Yang zeros and edge singularity in a mean-field approach","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2509.19009","citing_title":"Finite-temperature Yang-Mills theories with the density of states method: towards the continuum limit","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IU4QUEI6XGHYP4XZUSHXHANY2F","json":"https://pith.science/pith/IU4QUEI6XGHYP4XZUSHXHANY2F.json","graph_json":"https://pith.science/api/pith-number/IU4QUEI6XGHYP4XZUSHXHANY2F/graph.json","events_json":"https://pith.science/api/pith-number/IU4QUEI6XGHYP4XZUSHXHANY2F/events.json","paper":"https://pith.science/paper/IU4QUEI6"},"agent_actions":{"view_html":"https://pith.science/pith/IU4QUEI6XGHYP4XZUSHXHANY2F","download_json":"https://pith.science/pith/IU4QUEI6XGHYP4XZUSHXHANY2F.json","view_paper":"https://pith.science/paper/IU4QUEI6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2009.14033&json=true","fetch_graph":"https://pith.science/api/pith-number/IU4QUEI6XGHYP4XZUSHXHANY2F/graph.json","fetch_events":"https://pith.science/api/pith-number/IU4QUEI6XGHYP4XZUSHXHANY2F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IU4QUEI6XGHYP4XZUSHXHANY2F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IU4QUEI6XGHYP4XZUSHXHANY2F/action/storage_attestation","attest_author":"https://pith.science/pith/IU4QUEI6XGHYP4XZUSHXHANY2F/action/author_attestation","sign_citation":"https://pith.science/pith/IU4QUEI6XGHYP4XZUSHXHANY2F/action/citation_signature","submit_replication":"https://pith.science/pith/IU4QUEI6XGHYP4XZUSHXHANY2F/action/replication_record"}},"created_at":"2026-07-05T02:08:50.596214+00:00","updated_at":"2026-07-05T02:08:50.596214+00:00"}