{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:GZKD65NIMZVCE7QPFYTXEWF66C","short_pith_number":"pith:GZKD65NI","schema_version":"1.0","canonical_sha256":"36543f75a8666a227e0f2e277258bef0bf0dcdafbf7cd0db451f0325a90136bd","source":{"kind":"arxiv","id":"2308.10054","version":2},"attestation_state":"computed","paper":{"title":"Glueball Spectrum with four light dynamical fermions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-ph"],"primary_cat":"hep-lat","authors_text":"Adam Lantos, Andreas Athenodorou, Jacob Finkenrath, Michael Teper","submitted_at":"2023-08-19T15:32:25Z","abstract_excerpt":"We perform a calculation of the glueball spectrum for $N_f=4$ degenerate dynamical fermions with masses corresponding to light pions. We do so by making use of ensembles produced within the framework of maximally twisted fermions by the Extended Twisted Mass Collaboration (ETMC). We obtain masses of states that fall into the irreducible representations of the octahedral group of rotations in combination with the quantum numbers of charge conjugation $C$ and parity $P$; the above quantum numbers result in 20 distinct irreducible representations. We implement the Generalized Eigenvalue Problem ("},"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":"2308.10054","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2023-08-19T15:32:25Z","cross_cats_sorted":["hep-ex","hep-ph"],"title_canon_sha256":"3aef221d4a0c58e561c21683f64b2b157b49b1928f0129eaeeb4bf67eefc2097","abstract_canon_sha256":"a61dd1c9b126395f39858aef856747727befdcaa27cb8e1bc97631900e0972d7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:13:44.033751Z","signature_b64":"LXkxoSw1TWE4eUSEc/JWEptTrTuuYhRaiDhcI22VdjutJNfKQOiLyL9+frwlzc9AHcKGJ/2ZEe3+Gu19Bu2dAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"36543f75a8666a227e0f2e277258bef0bf0dcdafbf7cd0db451f0325a90136bd","last_reissued_at":"2026-07-05T07:13:44.033323Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:13:44.033323Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Glueball Spectrum with four light dynamical fermions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-ph"],"primary_cat":"hep-lat","authors_text":"Adam Lantos, Andreas Athenodorou, Jacob Finkenrath, Michael Teper","submitted_at":"2023-08-19T15:32:25Z","abstract_excerpt":"We perform a calculation of the glueball spectrum for $N_f=4$ degenerate dynamical fermions with masses corresponding to light pions. We do so by making use of ensembles produced within the framework of maximally twisted fermions by the Extended Twisted Mass Collaboration (ETMC). We obtain masses of states that fall into the irreducible representations of the octahedral group of rotations in combination with the quantum numbers of charge conjugation $C$ and parity $P$; the above quantum numbers result in 20 distinct irreducible representations. We implement the Generalized Eigenvalue Problem ("},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2308.10054","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/2308.10054/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":"2308.10054","created_at":"2026-07-05T07:13:44.033380+00:00"},{"alias_kind":"arxiv_version","alias_value":"2308.10054v2","created_at":"2026-07-05T07:13:44.033380+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2308.10054","created_at":"2026-07-05T07:13:44.033380+00:00"},{"alias_kind":"pith_short_12","alias_value":"GZKD65NIMZVC","created_at":"2026-07-05T07:13:44.033380+00:00"},{"alias_kind":"pith_short_16","alias_value":"GZKD65NIMZVCE7QP","created_at":"2026-07-05T07:13:44.033380+00:00"},{"alias_kind":"pith_short_8","alias_value":"GZKD65NI","created_at":"2026-07-05T07:13:44.033380+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.01757","citing_title":"Production Rate of Glueball-like $X(2370)$ in $J/\\psi$ Radiative Decay","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GZKD65NIMZVCE7QPFYTXEWF66C","json":"https://pith.science/pith/GZKD65NIMZVCE7QPFYTXEWF66C.json","graph_json":"https://pith.science/api/pith-number/GZKD65NIMZVCE7QPFYTXEWF66C/graph.json","events_json":"https://pith.science/api/pith-number/GZKD65NIMZVCE7QPFYTXEWF66C/events.json","paper":"https://pith.science/paper/GZKD65NI"},"agent_actions":{"view_html":"https://pith.science/pith/GZKD65NIMZVCE7QPFYTXEWF66C","download_json":"https://pith.science/pith/GZKD65NIMZVCE7QPFYTXEWF66C.json","view_paper":"https://pith.science/paper/GZKD65NI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2308.10054&json=true","fetch_graph":"https://pith.science/api/pith-number/GZKD65NIMZVCE7QPFYTXEWF66C/graph.json","fetch_events":"https://pith.science/api/pith-number/GZKD65NIMZVCE7QPFYTXEWF66C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GZKD65NIMZVCE7QPFYTXEWF66C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GZKD65NIMZVCE7QPFYTXEWF66C/action/storage_attestation","attest_author":"https://pith.science/pith/GZKD65NIMZVCE7QPFYTXEWF66C/action/author_attestation","sign_citation":"https://pith.science/pith/GZKD65NIMZVCE7QPFYTXEWF66C/action/citation_signature","submit_replication":"https://pith.science/pith/GZKD65NIMZVCE7QPFYTXEWF66C/action/replication_record"}},"created_at":"2026-07-05T07:13:44.033380+00:00","updated_at":"2026-07-05T07:13:44.033380+00:00"}