{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:YU34X2CBZO5ZWNJ4ODUDGWEWLB","short_pith_number":"pith:YU34X2CB","schema_version":"1.0","canonical_sha256":"c537cbe841cbbb9b353c70e8335896585c6061faa53f03e9855d6ba6581102e5","source":{"kind":"arxiv","id":"1611.07370","version":1},"attestation_state":"computed","paper":{"title":"Finite-volume effects on phase transition in the Polyakov-loop extended Nambu-Jona-Lasinio model with a chiral chemical potential","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Chao-Hsi Chang, Hong-shi Zong, Zan Pan, Zhu-Fang Cui","submitted_at":"2016-11-22T15:41:26Z","abstract_excerpt":"To investigate finite-volume effects on the chiral symmetry restoration and the deconfinement transition and some impacts of possible global topological background for a quantum chromodynamics (QCD) system with $N_f=2$ (two quark flavors), we apply the Polyakov-loop extended Nambu-Jona-Lasinio model by introducing a chiral chemical potential $\\mu_5$ artificially. The final numerical results indicate that the introduced chiral chemical potential does not change the critical exponents but shifts the location of critical end point (CEP) significantly; the ratios for the chiral chemical potentials"},"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":"1611.07370","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-22T15:41:26Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"d331428fd154a7feea5e87123202688f31fb25ecbf4076a05d6486b98f1297f0","abstract_canon_sha256":"7426f37ef88c5603a6d16a91e62d12126f75b1cfd7049cecc62ee59535d16d23"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:38.877897Z","signature_b64":"LzRPB5xWCqtpLU6/tPVpYYsWWNpk39gzJLMNAAOwgZvw0yISzV8dhzrFG2ZzLiAwn0B0iUYGeYJPoprtF/8dAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c537cbe841cbbb9b353c70e8335896585c6061faa53f03e9855d6ba6581102e5","last_reissued_at":"2026-05-18T00:46:38.877311Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:38.877311Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite-volume effects on phase transition in the Polyakov-loop extended Nambu-Jona-Lasinio model with a chiral chemical potential","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Chao-Hsi Chang, Hong-shi Zong, Zan Pan, Zhu-Fang Cui","submitted_at":"2016-11-22T15:41:26Z","abstract_excerpt":"To investigate finite-volume effects on the chiral symmetry restoration and the deconfinement transition and some impacts of possible global topological background for a quantum chromodynamics (QCD) system with $N_f=2$ (two quark flavors), we apply the Polyakov-loop extended Nambu-Jona-Lasinio model by introducing a chiral chemical potential $\\mu_5$ artificially. The final numerical results indicate that the introduced chiral chemical potential does not change the critical exponents but shifts the location of critical end point (CEP) significantly; the ratios for the chiral chemical potentials"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.07370","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":""},"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":"1611.07370","created_at":"2026-05-18T00:46:38.877418+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.07370v1","created_at":"2026-05-18T00:46:38.877418+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.07370","created_at":"2026-05-18T00:46:38.877418+00:00"},{"alias_kind":"pith_short_12","alias_value":"YU34X2CBZO5Z","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_16","alias_value":"YU34X2CBZO5ZWNJ4","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_8","alias_value":"YU34X2CB","created_at":"2026-05-18T12:30:53.716459+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.19964","citing_title":"Lee-Yang zeros and edge singularity in a mean-field approach","ref_index":53,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YU34X2CBZO5ZWNJ4ODUDGWEWLB","json":"https://pith.science/pith/YU34X2CBZO5ZWNJ4ODUDGWEWLB.json","graph_json":"https://pith.science/api/pith-number/YU34X2CBZO5ZWNJ4ODUDGWEWLB/graph.json","events_json":"https://pith.science/api/pith-number/YU34X2CBZO5ZWNJ4ODUDGWEWLB/events.json","paper":"https://pith.science/paper/YU34X2CB"},"agent_actions":{"view_html":"https://pith.science/pith/YU34X2CBZO5ZWNJ4ODUDGWEWLB","download_json":"https://pith.science/pith/YU34X2CBZO5ZWNJ4ODUDGWEWLB.json","view_paper":"https://pith.science/paper/YU34X2CB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.07370&json=true","fetch_graph":"https://pith.science/api/pith-number/YU34X2CBZO5ZWNJ4ODUDGWEWLB/graph.json","fetch_events":"https://pith.science/api/pith-number/YU34X2CBZO5ZWNJ4ODUDGWEWLB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YU34X2CBZO5ZWNJ4ODUDGWEWLB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YU34X2CBZO5ZWNJ4ODUDGWEWLB/action/storage_attestation","attest_author":"https://pith.science/pith/YU34X2CBZO5ZWNJ4ODUDGWEWLB/action/author_attestation","sign_citation":"https://pith.science/pith/YU34X2CBZO5ZWNJ4ODUDGWEWLB/action/citation_signature","submit_replication":"https://pith.science/pith/YU34X2CBZO5ZWNJ4ODUDGWEWLB/action/replication_record"}},"created_at":"2026-05-18T00:46:38.877418+00:00","updated_at":"2026-05-18T00:46:38.877418+00:00"}