{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:RB72NSTKSDOEEKNCCVKZIOJ4AB","short_pith_number":"pith:RB72NSTK","schema_version":"1.0","canonical_sha256":"887fa6ca6a90dc4229a2155594393c00752741470e5854f3a665bf87e2180ef4","source":{"kind":"arxiv","id":"2608.03362","version":1},"attestation_state":"computed","paper":{"title":"Analysis of the $X(2370)$ as a glueball based on rigorous current-field duality","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Zhi-Gang Wang","submitted_at":"2026-08-04T09:09:56Z","abstract_excerpt":"In this work, we take the $X(2370)$ with $J^{PC}=0^{-+}$ as a glueball consists of three valence gluons, and construct a six-quark current based on rigorous current-field duality to obtain the glueball-quark Lagrangian. Then we perform Fierz transformation to bosonize the quark current into a series of three pseudoscalar mesons. At last, we obtain ratios among the partial decay widths of the glueball to three pseudoscalar mesons in a model-independent way, which are compatible with the experimental data from the BESIII Collaboration and support assigning the $X(2370)$ as a glueball."},"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":"2608.03362","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-08-04T09:09:56Z","cross_cats_sorted":[],"title_canon_sha256":"7d1c21a7bb379b3aa1268d80fe8d88334c68e41925f4086e70e02aecfe9aaac8","abstract_canon_sha256":"e849ec934bba42598cfc1fe9d335aa326b84051839df48f14dcc4ff44105df82"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-05T00:47:00.713138Z","signature_b64":"gbFl2EbChRPZHYXQUsZiFETNfHBvPa/+hKX+Q+rOCaFJ5LnWO6egCCPgb+nFmjvQW9Jx9/Hfyo+Iggp+N42yBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"887fa6ca6a90dc4229a2155594393c00752741470e5854f3a665bf87e2180ef4","last_reissued_at":"2026-08-05T00:47:00.710560Z","signature_status":"signed_v1","first_computed_at":"2026-08-05T00:47:00.710560Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis of the $X(2370)$ as a glueball based on rigorous current-field duality","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Zhi-Gang Wang","submitted_at":"2026-08-04T09:09:56Z","abstract_excerpt":"In this work, we take the $X(2370)$ with $J^{PC}=0^{-+}$ as a glueball consists of three valence gluons, and construct a six-quark current based on rigorous current-field duality to obtain the glueball-quark Lagrangian. Then we perform Fierz transformation to bosonize the quark current into a series of three pseudoscalar mesons. At last, we obtain ratios among the partial decay widths of the glueball to three pseudoscalar mesons in a model-independent way, which are compatible with the experimental data from the BESIII Collaboration and support assigning the $X(2370)$ as a glueball."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.03362","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2608.03362/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":"2608.03362","created_at":"2026-08-05T00:47:00.711405+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.03362v1","created_at":"2026-08-05T00:47:00.711405+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.03362","created_at":"2026-08-05T00:47:00.711405+00:00"},{"alias_kind":"pith_short_12","alias_value":"RB72NSTKSDOE","created_at":"2026-08-05T00:47:00.711405+00:00"},{"alias_kind":"pith_short_16","alias_value":"RB72NSTKSDOEEKNC","created_at":"2026-08-05T00:47:00.711405+00:00"},{"alias_kind":"pith_short_8","alias_value":"RB72NSTK","created_at":"2026-08-05T00:47:00.711405+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.11814","citing_title":"The decay properties of two- and three- gluon glueballs","ref_index":54,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RB72NSTKSDOEEKNCCVKZIOJ4AB","json":"https://pith.science/pith/RB72NSTKSDOEEKNCCVKZIOJ4AB.json","graph_json":"https://pith.science/api/pith-number/RB72NSTKSDOEEKNCCVKZIOJ4AB/graph.json","events_json":"https://pith.science/api/pith-number/RB72NSTKSDOEEKNCCVKZIOJ4AB/events.json","paper":"https://pith.science/paper/RB72NSTK"},"agent_actions":{"view_html":"https://pith.science/pith/RB72NSTKSDOEEKNCCVKZIOJ4AB","download_json":"https://pith.science/pith/RB72NSTKSDOEEKNCCVKZIOJ4AB.json","view_paper":"https://pith.science/paper/RB72NSTK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.03362&json=true","fetch_graph":"https://pith.science/api/pith-number/RB72NSTKSDOEEKNCCVKZIOJ4AB/graph.json","fetch_events":"https://pith.science/api/pith-number/RB72NSTKSDOEEKNCCVKZIOJ4AB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RB72NSTKSDOEEKNCCVKZIOJ4AB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RB72NSTKSDOEEKNCCVKZIOJ4AB/action/storage_attestation","attest_author":"https://pith.science/pith/RB72NSTKSDOEEKNCCVKZIOJ4AB/action/author_attestation","sign_citation":"https://pith.science/pith/RB72NSTKSDOEEKNCCVKZIOJ4AB/action/citation_signature","submit_replication":"https://pith.science/pith/RB72NSTKSDOEEKNCCVKZIOJ4AB/action/replication_record"}},"created_at":"2026-08-05T00:47:00.711405+00:00","updated_at":"2026-08-05T00:47:00.711405+00:00"}