{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:LWKGOTA5LMJY2ZPLJME53RS2V7","short_pith_number":"pith:LWKGOTA5","schema_version":"1.0","canonical_sha256":"5d94674c1d5b138d65eb4b09ddc65aafc882ed069e4806929c69d911c982319d","source":{"kind":"arxiv","id":"2307.05755","version":1},"attestation_state":"computed","paper":{"title":"QCD on Rotating Lattice with Staggered Fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th","nucl-th"],"primary_cat":"hep-lat","authors_text":"Ji-Chong Yang, Xu-Guang Huang","submitted_at":"2023-07-11T19:21:37Z","abstract_excerpt":"We investigate the finite-temperature quantum chromodynamics (QCD) on a rotating lattice with $N_f=2+1$ staggered fermions and the projective plane boundary condition. We observe a negative rotational rigidity (defined in the main text) and a negative quark spin susceptibility associated with the chiral vortical effect. In contrast to most of the effective model predictions, we find that the chiral condensate decreases and the Polyakov loop increases with imaginary rotation, implying a rotational catalysis of chiral symmetry breaking and confinement by real rotation. We determine the phase bou"},"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":"2307.05755","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2023-07-11T19:21:37Z","cross_cats_sorted":["hep-ph","hep-th","nucl-th"],"title_canon_sha256":"8d2b4a7777b04ced7f4022765be93d2c8ec3de5195453be17808e23909c16c5f","abstract_canon_sha256":"a8fc72b3166aa31700bc8816aa529f24326cc85aa849a60efd924eaeed08c2a2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:30:11.942073Z","signature_b64":"2ebN0X72WP3qYVHDLQ2l4cOh9srqjYmSwD3liSW6blU45/mA+AtsBdudNIWC714iFlsu5MxdNETrRdDeZ8OCDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d94674c1d5b138d65eb4b09ddc65aafc882ed069e4806929c69d911c982319d","last_reissued_at":"2026-07-05T06:30:11.941648Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:30:11.941648Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"QCD on Rotating Lattice with Staggered Fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th","nucl-th"],"primary_cat":"hep-lat","authors_text":"Ji-Chong Yang, Xu-Guang Huang","submitted_at":"2023-07-11T19:21:37Z","abstract_excerpt":"We investigate the finite-temperature quantum chromodynamics (QCD) on a rotating lattice with $N_f=2+1$ staggered fermions and the projective plane boundary condition. We observe a negative rotational rigidity (defined in the main text) and a negative quark spin susceptibility associated with the chiral vortical effect. In contrast to most of the effective model predictions, we find that the chiral condensate decreases and the Polyakov loop increases with imaginary rotation, implying a rotational catalysis of chiral symmetry breaking and confinement by real rotation. We determine the phase bou"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.05755","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2307.05755/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":"2307.05755","created_at":"2026-07-05T06:30:11.941703+00:00"},{"alias_kind":"arxiv_version","alias_value":"2307.05755v1","created_at":"2026-07-05T06:30:11.941703+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.05755","created_at":"2026-07-05T06:30:11.941703+00:00"},{"alias_kind":"pith_short_12","alias_value":"LWKGOTA5LMJY","created_at":"2026-07-05T06:30:11.941703+00:00"},{"alias_kind":"pith_short_16","alias_value":"LWKGOTA5LMJY2ZPL","created_at":"2026-07-05T06:30:11.941703+00:00"},{"alias_kind":"pith_short_8","alias_value":"LWKGOTA5","created_at":"2026-07-05T06:30:11.941703+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2503.17291","citing_title":"Linear sigma model with quarks and Polyakov loop in rotation: phase diagrams, Tolman-Ehrenfest law and mechanical properties","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2602.20970","citing_title":"Spatial confinement-deconfinement transition in accelerated gluodynamics within lattice simulation","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2602.23094","citing_title":"Spatially inhomogeneous confinement-deconfinement phase transition in rotating QGP","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2604.06248","citing_title":"Relativistic Barnett effect and Curie law in a rigidly rotating free Fermi gas","ref_index":35,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LWKGOTA5LMJY2ZPLJME53RS2V7","json":"https://pith.science/pith/LWKGOTA5LMJY2ZPLJME53RS2V7.json","graph_json":"https://pith.science/api/pith-number/LWKGOTA5LMJY2ZPLJME53RS2V7/graph.json","events_json":"https://pith.science/api/pith-number/LWKGOTA5LMJY2ZPLJME53RS2V7/events.json","paper":"https://pith.science/paper/LWKGOTA5"},"agent_actions":{"view_html":"https://pith.science/pith/LWKGOTA5LMJY2ZPLJME53RS2V7","download_json":"https://pith.science/pith/LWKGOTA5LMJY2ZPLJME53RS2V7.json","view_paper":"https://pith.science/paper/LWKGOTA5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2307.05755&json=true","fetch_graph":"https://pith.science/api/pith-number/LWKGOTA5LMJY2ZPLJME53RS2V7/graph.json","fetch_events":"https://pith.science/api/pith-number/LWKGOTA5LMJY2ZPLJME53RS2V7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LWKGOTA5LMJY2ZPLJME53RS2V7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LWKGOTA5LMJY2ZPLJME53RS2V7/action/storage_attestation","attest_author":"https://pith.science/pith/LWKGOTA5LMJY2ZPLJME53RS2V7/action/author_attestation","sign_citation":"https://pith.science/pith/LWKGOTA5LMJY2ZPLJME53RS2V7/action/citation_signature","submit_replication":"https://pith.science/pith/LWKGOTA5LMJY2ZPLJME53RS2V7/action/replication_record"}},"created_at":"2026-07-05T06:30:11.941703+00:00","updated_at":"2026-07-05T06:30:11.941703+00:00"}