{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:AIGHODVKRJHKVWJ7YFD3K5U2BJ","short_pith_number":"pith:AIGHODVK","schema_version":"1.0","canonical_sha256":"020c770eaa8a4eaad93fc147b5769a0a558f4a5bbb84405701ac6935f403d2b1","source":{"kind":"arxiv","id":"0808.3151","version":1},"attestation_state":"computed","paper":{"title":"Glueball matrix elements: a lattice calculation and applications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Harvey B. Meyer","submitted_at":"2008-08-22T21:46:03Z","abstract_excerpt":"We compute the matrix elements of the energy-momentum tensor between glueball states and the vacuum in SU(3) lattice gauge theory and extrapolate them to the continuum. These matrix elements may play an important phenomenological role in identifying glue-rich mesons. Based on a relation derived long ago by the ITEP group for J/psi radiative decays, the scalar matrix element leads to a branching ratio for the glueball that is at least three times larger than the experimentally observed branching ratio for the f_0 mesons above 1GeV. This suggests that the glueball component must be diluted quite"},"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":"0808.3151","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2008-08-22T21:46:03Z","cross_cats_sorted":[],"title_canon_sha256":"c45842543796c5e281feec91bd87545930e6e9063fb2a2c48a9bff463f69ccfd","abstract_canon_sha256":"52d16324ed1eaa4d0b0a1c70c413c6096b109fd7805b329b751f5ebb1a4964a0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:37:05.521023Z","signature_b64":"ToxV/qUJ8e9CfEwNO31Rr7dqK38LkJjCmbIFaI7jBqUbi24oSZ32nYpLFjgpIZqK0PCPmljrg8X3tMcP1HSkDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"020c770eaa8a4eaad93fc147b5769a0a558f4a5bbb84405701ac6935f403d2b1","last_reissued_at":"2026-07-04T15:37:05.520647Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:37:05.520647Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Glueball matrix elements: a lattice calculation and applications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Harvey B. Meyer","submitted_at":"2008-08-22T21:46:03Z","abstract_excerpt":"We compute the matrix elements of the energy-momentum tensor between glueball states and the vacuum in SU(3) lattice gauge theory and extrapolate them to the continuum. These matrix elements may play an important phenomenological role in identifying glue-rich mesons. Based on a relation derived long ago by the ITEP group for J/psi radiative decays, the scalar matrix element leads to a branching ratio for the glueball that is at least three times larger than the experimentally observed branching ratio for the f_0 mesons above 1GeV. This suggests that the glueball component must be diluted quite"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0808.3151","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/0808.3151/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":"0808.3151","created_at":"2026-07-04T15:37:05.520713+00:00"},{"alias_kind":"arxiv_version","alias_value":"0808.3151v1","created_at":"2026-07-04T15:37:05.520713+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0808.3151","created_at":"2026-07-04T15:37:05.520713+00:00"},{"alias_kind":"pith_short_12","alias_value":"AIGHODVKRJHK","created_at":"2026-07-04T15:37:05.520713+00:00"},{"alias_kind":"pith_short_16","alias_value":"AIGHODVKRJHKVWJ7","created_at":"2026-07-04T15:37:05.520713+00:00"},{"alias_kind":"pith_short_8","alias_value":"AIGHODVK","created_at":"2026-07-04T15:37:05.520713+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.09794","citing_title":"Optical gravitational waves as signals of Gravitationally-Decaying Particles","ref_index":49,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AIGHODVKRJHKVWJ7YFD3K5U2BJ","json":"https://pith.science/pith/AIGHODVKRJHKVWJ7YFD3K5U2BJ.json","graph_json":"https://pith.science/api/pith-number/AIGHODVKRJHKVWJ7YFD3K5U2BJ/graph.json","events_json":"https://pith.science/api/pith-number/AIGHODVKRJHKVWJ7YFD3K5U2BJ/events.json","paper":"https://pith.science/paper/AIGHODVK"},"agent_actions":{"view_html":"https://pith.science/pith/AIGHODVKRJHKVWJ7YFD3K5U2BJ","download_json":"https://pith.science/pith/AIGHODVKRJHKVWJ7YFD3K5U2BJ.json","view_paper":"https://pith.science/paper/AIGHODVK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0808.3151&json=true","fetch_graph":"https://pith.science/api/pith-number/AIGHODVKRJHKVWJ7YFD3K5U2BJ/graph.json","fetch_events":"https://pith.science/api/pith-number/AIGHODVKRJHKVWJ7YFD3K5U2BJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AIGHODVKRJHKVWJ7YFD3K5U2BJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AIGHODVKRJHKVWJ7YFD3K5U2BJ/action/storage_attestation","attest_author":"https://pith.science/pith/AIGHODVKRJHKVWJ7YFD3K5U2BJ/action/author_attestation","sign_citation":"https://pith.science/pith/AIGHODVKRJHKVWJ7YFD3K5U2BJ/action/citation_signature","submit_replication":"https://pith.science/pith/AIGHODVKRJHKVWJ7YFD3K5U2BJ/action/replication_record"}},"created_at":"2026-07-04T15:37:05.520713+00:00","updated_at":"2026-07-04T15:37:05.520713+00:00"}