{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:PCMMJQ6LTG4QLPQQYPGZVKH25Y","short_pith_number":"pith:PCMMJQ6L","schema_version":"1.0","canonical_sha256":"7898c4c3cb99b905be10c3cd9aa8faee2bfb194b8ba03f202f0ba55cb55d52e3","source":{"kind":"arxiv","id":"1508.07132","version":3},"attestation_state":"computed","paper":{"title":"Lattice study on QCD-like theory with exact center symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th","nucl-th"],"primary_cat":"hep-lat","authors_text":"Etsuko Itou, Takumi Iritani, Tatsuhiro Misumi","submitted_at":"2015-08-28T08:58:59Z","abstract_excerpt":"We investigate QCD-like theory with exact center symmetry, with emphasis on the finite-temperature phase transition concerning center and chiral symmetries. On the lattice, we formulate center symmetric $SU(3)$ gauge theory with three fundamental Wilson quarks by twisting quark boundary conditions in a compact direction ($Z_3$-QCD model). We calculate the expectation value of Polyakov loop and the chiral condensate as a function of temperature on 16^3 x 4 and 20^3 x 4 lattices along the line of constant physics realizing $m_{PS}/m_{V}=0.70$. We find out the first-order center phase transition,"},"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":"1508.07132","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-08-28T08:58:59Z","cross_cats_sorted":["hep-ph","hep-th","nucl-th"],"title_canon_sha256":"a02e17afb52ab4568e224e51365aa968f316e5416cd332eba7b53d2f1e1adcbe","abstract_canon_sha256":"256d59c00d255bfd7b2a5cc6328783539c78ec92415068eaf80161e6051e8fe7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:25:54.976898Z","signature_b64":"udPg3tQaZR3y1scQ0hMBn3e6J7SFXTsTX/mVZny5r4tcbb7EEYdJa4ICWPpAdH1WQDH1BOctU1DOb80rJAHQCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7898c4c3cb99b905be10c3cd9aa8faee2bfb194b8ba03f202f0ba55cb55d52e3","last_reissued_at":"2026-05-18T01:25:54.976176Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:25:54.976176Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lattice study on QCD-like theory with exact center symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th","nucl-th"],"primary_cat":"hep-lat","authors_text":"Etsuko Itou, Takumi Iritani, Tatsuhiro Misumi","submitted_at":"2015-08-28T08:58:59Z","abstract_excerpt":"We investigate QCD-like theory with exact center symmetry, with emphasis on the finite-temperature phase transition concerning center and chiral symmetries. On the lattice, we formulate center symmetric $SU(3)$ gauge theory with three fundamental Wilson quarks by twisting quark boundary conditions in a compact direction ($Z_3$-QCD model). We calculate the expectation value of Polyakov loop and the chiral condensate as a function of temperature on 16^3 x 4 and 20^3 x 4 lattices along the line of constant physics realizing $m_{PS}/m_{V}=0.70$. We find out the first-order center phase transition,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.07132","kind":"arxiv","version":3},"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":"1508.07132","created_at":"2026-05-18T01:25:54.976288+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.07132v3","created_at":"2026-05-18T01:25:54.976288+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.07132","created_at":"2026-05-18T01:25:54.976288+00:00"},{"alias_kind":"pith_short_12","alias_value":"PCMMJQ6LTG4Q","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_16","alias_value":"PCMMJQ6LTG4QLPQQ","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_8","alias_value":"PCMMJQ6L","created_at":"2026-05-18T12:29:37.295048+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.17848","citing_title":"Adiabatic continuity in a partially reduced twisted Eguchi-Kawai model with one adjoint Dirac fermion","ref_index":73,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PCMMJQ6LTG4QLPQQYPGZVKH25Y","json":"https://pith.science/pith/PCMMJQ6LTG4QLPQQYPGZVKH25Y.json","graph_json":"https://pith.science/api/pith-number/PCMMJQ6LTG4QLPQQYPGZVKH25Y/graph.json","events_json":"https://pith.science/api/pith-number/PCMMJQ6LTG4QLPQQYPGZVKH25Y/events.json","paper":"https://pith.science/paper/PCMMJQ6L"},"agent_actions":{"view_html":"https://pith.science/pith/PCMMJQ6LTG4QLPQQYPGZVKH25Y","download_json":"https://pith.science/pith/PCMMJQ6LTG4QLPQQYPGZVKH25Y.json","view_paper":"https://pith.science/paper/PCMMJQ6L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.07132&json=true","fetch_graph":"https://pith.science/api/pith-number/PCMMJQ6LTG4QLPQQYPGZVKH25Y/graph.json","fetch_events":"https://pith.science/api/pith-number/PCMMJQ6LTG4QLPQQYPGZVKH25Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PCMMJQ6LTG4QLPQQYPGZVKH25Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PCMMJQ6LTG4QLPQQYPGZVKH25Y/action/storage_attestation","attest_author":"https://pith.science/pith/PCMMJQ6LTG4QLPQQYPGZVKH25Y/action/author_attestation","sign_citation":"https://pith.science/pith/PCMMJQ6LTG4QLPQQYPGZVKH25Y/action/citation_signature","submit_replication":"https://pith.science/pith/PCMMJQ6LTG4QLPQQYPGZVKH25Y/action/replication_record"}},"created_at":"2026-05-18T01:25:54.976288+00:00","updated_at":"2026-05-18T01:25:54.976288+00:00"}