{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:RML3RRWAUFQS35FIAZJBVDT45W","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"f12c71b9f91f980640016e83d90f56a7571a0cacb99c1dce6e5136a87c92d811","cross_cats_sorted":["hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2022-10-15T00:55:30Z","title_canon_sha256":"e2e2706c7bfa7262e644f12f09afe1d85ab87277977bacded1634993d203411a"},"schema_version":"1.0","source":{"id":"2210.08154","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.08154","created_at":"2026-07-05T05:07:07Z"},{"alias_kind":"arxiv_version","alias_value":"2210.08154v1","created_at":"2026-07-05T05:07:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.08154","created_at":"2026-07-05T05:07:07Z"},{"alias_kind":"pith_short_12","alias_value":"RML3RRWAUFQS","created_at":"2026-07-05T05:07:07Z"},{"alias_kind":"pith_short_16","alias_value":"RML3RRWAUFQS35FI","created_at":"2026-07-05T05:07:07Z"},{"alias_kind":"pith_short_8","alias_value":"RML3RRWA","created_at":"2026-07-05T05:07:07Z"}],"graph_snapshots":[{"event_id":"sha256:187500e4ec798734e8bd3d18bab658baea4cd848291bb5dbc39e21f988796009","target":"graph","created_at":"2026-07-05T05:07:07Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2210.08154/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We perform numerical calculations of masses and decay constants of the lightest (flavoured) pseudoscalar, vector and axial vector mesons in the $Sp(4)$ lattice gauge theory with three Dirac fermions in the antisymmetric representation. The corresponding continuum theory plays an important role in certain ultra-violet complete realisations of composite Higgs, partial top compositeness, and composite dark matter models. In addition, we measure the masses of other flavoured mesons in spin-$0$ and $1$ channels, as well as the first excited state of the vector mesons. Using the gradient flow to set","authors_text":"Biagio Lucini, C.-J. David Lin, Davide Vadacchino, Deog Ki Hong, Ed Bennett, Ho Hsiao, Jong-Wan Lee, Maurizio Piai","cross_cats":["hep-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2022-10-15T00:55:30Z","title":"Spectroscopy of $Sp(4)$ lattice gauge theory with $n_f=3$ antisymmetric fermions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.08154","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:f6f00593f4b3c7def2d109f385787c7f2ef1648feadd69235e008a6c2d7847a8","target":"record","created_at":"2026-07-05T05:07:07Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"f12c71b9f91f980640016e83d90f56a7571a0cacb99c1dce6e5136a87c92d811","cross_cats_sorted":["hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2022-10-15T00:55:30Z","title_canon_sha256":"e2e2706c7bfa7262e644f12f09afe1d85ab87277977bacded1634993d203411a"},"schema_version":"1.0","source":{"id":"2210.08154","kind":"arxiv","version":1}},"canonical_sha256":"8b17b8c6c0a1612df4a806521a8e7ceda99d5a808e10a09030cee598ed0798d4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8b17b8c6c0a1612df4a806521a8e7ceda99d5a808e10a09030cee598ed0798d4","first_computed_at":"2026-07-05T05:07:07.775584Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:07:07.775584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BlsiSdv45N6JV5IaAOjrwXITIWvMiVER8pBrTBkNKMsLtmx89ctvPU6witIyvH/WYLpy4Jn1HQz7JDaRKykXDA==","signature_status":"signed_v1","signed_at":"2026-07-05T05:07:07.776073Z","signed_message":"canonical_sha256_bytes"},"source_id":"2210.08154","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f6f00593f4b3c7def2d109f385787c7f2ef1648feadd69235e008a6c2d7847a8","sha256:187500e4ec798734e8bd3d18bab658baea4cd848291bb5dbc39e21f988796009"],"state_sha256":"62debb88d8faca8e25ab0c8e29c41f74b5e02020cc215d92d818ce336793608f"}