{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:FHU24PNJ4OBFWDEDX4MHNFFZR4","short_pith_number":"pith:FHU24PNJ","schema_version":"1.0","canonical_sha256":"29e9ae3da9e3825b0c83bf187694b98f2e48bfbfea73037d69203af05b1ddd03","source":{"kind":"arxiv","id":"1707.01881","version":3},"attestation_state":"computed","paper":{"title":"Approximate degeneracy of $J=1$ spatial correlators in high temperature QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"C. B. Lang, C. Rohrhofer, G. Cossu, H. Fukaya, L. Ya. Glozman, S. Hashimoto, S. Prelovsek, Y. Aoki","submitted_at":"2017-07-06T17:39:18Z","abstract_excerpt":"We study spatial isovector meson correlators in $N_f=2$ QCD with dynamical domain-wall fermions on $32^3\\times 8$ lattices at temperatures $T=220-380$ MeV. We measure the correlators of spin-one ($J=1$) operators including vector, axial-vector, tensor and axial-tensor. Restoration of chiral $U(1)_A$ and $SU(2)_L \\times SU(2)_R$ symmetries of QCD implies degeneracies in vector--axial-vector ($SU(2)_L \\times SU(2)_R$) and tensor--axial-tensor ($U(1)_A$) pairs, which are indeed observed at temperatures above $T_c$. Moreover, we observe an approximate degeneracy of all $J=1$ correlators with incre"},"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":"1707.01881","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-07-06T17:39:18Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"f0552868f43af5955b5b2429be3bf49a901ec18eb1d814ffedb96b6a8f5ec374","abstract_canon_sha256":"5e723cac6a2451c698dde8c9a27b206fcece693caf4aec6f8aa60c9710fc6383"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:54:28.380671Z","signature_b64":"utnfBzCUurP0A404IZBMvp+e8WnnQMkv8crjvfjsTo/IXqjsvoaJ9aPneDd5rQu0LTEOCHsFJPZEtr1k0uMLBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"29e9ae3da9e3825b0c83bf187694b98f2e48bfbfea73037d69203af05b1ddd03","last_reissued_at":"2026-05-17T23:54:28.380210Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:54:28.380210Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Approximate degeneracy of $J=1$ spatial correlators in high temperature QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"C. B. Lang, C. Rohrhofer, G. Cossu, H. Fukaya, L. Ya. Glozman, S. Hashimoto, S. Prelovsek, Y. Aoki","submitted_at":"2017-07-06T17:39:18Z","abstract_excerpt":"We study spatial isovector meson correlators in $N_f=2$ QCD with dynamical domain-wall fermions on $32^3\\times 8$ lattices at temperatures $T=220-380$ MeV. We measure the correlators of spin-one ($J=1$) operators including vector, axial-vector, tensor and axial-tensor. Restoration of chiral $U(1)_A$ and $SU(2)_L \\times SU(2)_R$ symmetries of QCD implies degeneracies in vector--axial-vector ($SU(2)_L \\times SU(2)_R$) and tensor--axial-tensor ($U(1)_A$) pairs, which are indeed observed at temperatures above $T_c$. Moreover, we observe an approximate degeneracy of all $J=1$ correlators with incre"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.01881","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":"1707.01881","created_at":"2026-05-17T23:54:28.380288+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.01881v3","created_at":"2026-05-17T23:54:28.380288+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.01881","created_at":"2026-05-17T23:54:28.380288+00:00"},{"alias_kind":"pith_short_12","alias_value":"FHU24PNJ4OBF","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_16","alias_value":"FHU24PNJ4OBFWDED","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_8","alias_value":"FHU24PNJ","created_at":"2026-05-18T12:31:15.632608+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.23689","citing_title":"Three regimes/phases of QCD at high T, their symmetries and N_c scaling","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FHU24PNJ4OBFWDEDX4MHNFFZR4","json":"https://pith.science/pith/FHU24PNJ4OBFWDEDX4MHNFFZR4.json","graph_json":"https://pith.science/api/pith-number/FHU24PNJ4OBFWDEDX4MHNFFZR4/graph.json","events_json":"https://pith.science/api/pith-number/FHU24PNJ4OBFWDEDX4MHNFFZR4/events.json","paper":"https://pith.science/paper/FHU24PNJ"},"agent_actions":{"view_html":"https://pith.science/pith/FHU24PNJ4OBFWDEDX4MHNFFZR4","download_json":"https://pith.science/pith/FHU24PNJ4OBFWDEDX4MHNFFZR4.json","view_paper":"https://pith.science/paper/FHU24PNJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.01881&json=true","fetch_graph":"https://pith.science/api/pith-number/FHU24PNJ4OBFWDEDX4MHNFFZR4/graph.json","fetch_events":"https://pith.science/api/pith-number/FHU24PNJ4OBFWDEDX4MHNFFZR4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FHU24PNJ4OBFWDEDX4MHNFFZR4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FHU24PNJ4OBFWDEDX4MHNFFZR4/action/storage_attestation","attest_author":"https://pith.science/pith/FHU24PNJ4OBFWDEDX4MHNFFZR4/action/author_attestation","sign_citation":"https://pith.science/pith/FHU24PNJ4OBFWDEDX4MHNFFZR4/action/citation_signature","submit_replication":"https://pith.science/pith/FHU24PNJ4OBFWDEDX4MHNFFZR4/action/replication_record"}},"created_at":"2026-05-17T23:54:28.380288+00:00","updated_at":"2026-05-17T23:54:28.380288+00:00"}