{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:QHSVFBX2UW6D5FMQC5LUG7N6A4","short_pith_number":"pith:QHSVFBX2","schema_version":"1.0","canonical_sha256":"81e55286faa5bc3e95901757437dbe070cf0e74c74a6566bffd2bc28d0ab649a","source":{"kind":"arxiv","id":"2309.00086","version":2},"attestation_state":"computed","paper":{"title":"Anomalous interactions between mesons with nonzero spin and glueballs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Francesco Giacosa, Robert Pisarski, Shahriyar Jafarzade","submitted_at":"2023-08-31T18:56:56Z","abstract_excerpt":"Topologically nontrivial fluctuations control the anomalous interactions for the $\\eta$ and and $\\eta \\prime$ pseudoscalar mesons. We consider the anomalous interactions for mesons with higher spin, the heterochiral nonets with $J^{P C} = 1^{+ -}$ and $2^{- +}$. Under the approximation of a dilute gas of instantons, the mixing angle between non-strange and strange mesons decreases strongly as $J$ increases, and oscillates in sign. Anomalous interactions also open up new, rare decay channels. For glueballs, anomalous interactions indicate that the $X(2600)$ state is primarily gluonic."},"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":"2309.00086","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-08-31T18:56:56Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"a860efdf0eebacb68c771879c4aaac6464f1812408830d3d7dcd0b4cdd6be7be","abstract_canon_sha256":"94837c6ac412f6efa7a453c9eda5a52330c98a9b8af44d99885259064026569e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:56:42.767887Z","signature_b64":"M32Fc29eLZCIAXXF5j7ZkTmYR7M5qSuA2m4Zf+cuRr6PFmDRzcb+7hL8HAnKonY8nMJ4ZluUviMib72Sn+3UBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"81e55286faa5bc3e95901757437dbe070cf0e74c74a6566bffd2bc28d0ab649a","last_reissued_at":"2026-07-05T11:56:42.767410Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:56:42.767410Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomalous interactions between mesons with nonzero spin and glueballs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Francesco Giacosa, Robert Pisarski, Shahriyar Jafarzade","submitted_at":"2023-08-31T18:56:56Z","abstract_excerpt":"Topologically nontrivial fluctuations control the anomalous interactions for the $\\eta$ and and $\\eta \\prime$ pseudoscalar mesons. We consider the anomalous interactions for mesons with higher spin, the heterochiral nonets with $J^{P C} = 1^{+ -}$ and $2^{- +}$. Under the approximation of a dilute gas of instantons, the mixing angle between non-strange and strange mesons decreases strongly as $J$ increases, and oscillates in sign. Anomalous interactions also open up new, rare decay channels. For glueballs, anomalous interactions indicate that the $X(2600)$ state is primarily gluonic."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.00086","kind":"arxiv","version":2},"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/2309.00086/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":"2309.00086","created_at":"2026-07-05T11:56:42.767471+00:00"},{"alias_kind":"arxiv_version","alias_value":"2309.00086v2","created_at":"2026-07-05T11:56:42.767471+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.00086","created_at":"2026-07-05T11:56:42.767471+00:00"},{"alias_kind":"pith_short_12","alias_value":"QHSVFBX2UW6D","created_at":"2026-07-05T11:56:42.767471+00:00"},{"alias_kind":"pith_short_16","alias_value":"QHSVFBX2UW6D5FMQ","created_at":"2026-07-05T11:56:42.767471+00:00"},{"alias_kind":"pith_short_8","alias_value":"QHSVFBX2","created_at":"2026-07-05T11:56:42.767471+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.15704","citing_title":"Hidden-Strangeness Tetraquarks in the Dynamical Diquark Model","ref_index":62,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QHSVFBX2UW6D5FMQC5LUG7N6A4","json":"https://pith.science/pith/QHSVFBX2UW6D5FMQC5LUG7N6A4.json","graph_json":"https://pith.science/api/pith-number/QHSVFBX2UW6D5FMQC5LUG7N6A4/graph.json","events_json":"https://pith.science/api/pith-number/QHSVFBX2UW6D5FMQC5LUG7N6A4/events.json","paper":"https://pith.science/paper/QHSVFBX2"},"agent_actions":{"view_html":"https://pith.science/pith/QHSVFBX2UW6D5FMQC5LUG7N6A4","download_json":"https://pith.science/pith/QHSVFBX2UW6D5FMQC5LUG7N6A4.json","view_paper":"https://pith.science/paper/QHSVFBX2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2309.00086&json=true","fetch_graph":"https://pith.science/api/pith-number/QHSVFBX2UW6D5FMQC5LUG7N6A4/graph.json","fetch_events":"https://pith.science/api/pith-number/QHSVFBX2UW6D5FMQC5LUG7N6A4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QHSVFBX2UW6D5FMQC5LUG7N6A4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QHSVFBX2UW6D5FMQC5LUG7N6A4/action/storage_attestation","attest_author":"https://pith.science/pith/QHSVFBX2UW6D5FMQC5LUG7N6A4/action/author_attestation","sign_citation":"https://pith.science/pith/QHSVFBX2UW6D5FMQC5LUG7N6A4/action/citation_signature","submit_replication":"https://pith.science/pith/QHSVFBX2UW6D5FMQC5LUG7N6A4/action/replication_record"}},"created_at":"2026-07-05T11:56:42.767471+00:00","updated_at":"2026-07-05T11:56:42.767471+00:00"}