{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:L5FJH34UEYLXW7XAG2MPERI5RK","short_pith_number":"pith:L5FJH34U","schema_version":"1.0","canonical_sha256":"5f4a93ef9426177b7ee03698f2451d8a89dfa8ff87789f834e124be371b5976e","source":{"kind":"arxiv","id":"1301.5183","version":3},"attestation_state":"computed","paper":{"title":"The Status of Glueballs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Wolfgang Ochs","submitted_at":"2013-01-22T13:52:07Z","abstract_excerpt":"Calculations within QCD (lattice and sum rules) find the lightest glueball to be a scalar and with mass in the range of about 1000-1700 MeV. Several phenomenological investigations are discussed which aim at the identification of the scalar meson nonets of lowest mass and the super-numerous states if any. Results on the flavour structure of the light scalars f0(500), f0(980) and f0(1500) are presented; the evidence for f0(1370) is scrutinized. A significant surplus of leading clusters of neutral charge in gluon jets is found at LEP in comparison with MCs, possibly a direct signal for 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":"1301.5183","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-01-22T13:52:07Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"02c3563dd330207acbfeefa5fbbcfdbdef63dc87e3e13d3ff60ec8d0e75c6e00","abstract_canon_sha256":"16a6b34a6cc4e9387eda6a4f6fa5ab4199ba24dbaa8271569a9fbb6266bd3f2b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:31:44.465973Z","signature_b64":"/EpyAxrjeT6E3HMcb1N419+PlwtRyv+HHNhx/ssOaenBpKYVsMxSerQhY5aAUrcqroyD0flOGaEvbJfBlUOVBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5f4a93ef9426177b7ee03698f2451d8a89dfa8ff87789f834e124be371b5976e","last_reissued_at":"2026-05-18T03:31:44.465271Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:31:44.465271Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Status of Glueballs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Wolfgang Ochs","submitted_at":"2013-01-22T13:52:07Z","abstract_excerpt":"Calculations within QCD (lattice and sum rules) find the lightest glueball to be a scalar and with mass in the range of about 1000-1700 MeV. Several phenomenological investigations are discussed which aim at the identification of the scalar meson nonets of lowest mass and the super-numerous states if any. Results on the flavour structure of the light scalars f0(500), f0(980) and f0(1500) are presented; the evidence for f0(1370) is scrutinized. A significant surplus of leading clusters of neutral charge in gluon jets is found at LEP in comparison with MCs, possibly a direct signal for glueball "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.5183","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1301.5183","created_at":"2026-05-18T03:31:44.465394+00:00"},{"alias_kind":"arxiv_version","alias_value":"1301.5183v3","created_at":"2026-05-18T03:31:44.465394+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.5183","created_at":"2026-05-18T03:31:44.465394+00:00"},{"alias_kind":"pith_short_12","alias_value":"L5FJH34UEYLX","created_at":"2026-05-18T12:27:51.066281+00:00"},{"alias_kind":"pith_short_16","alias_value":"L5FJH34UEYLXW7XA","created_at":"2026-05-18T12:27:51.066281+00:00"},{"alias_kind":"pith_short_8","alias_value":"L5FJH34U","created_at":"2026-05-18T12:27:51.066281+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2607.02109","citing_title":"Light tetraquark states with $J^{PC}=1^{--}$ from QCD sum rules","ref_index":8,"is_internal_anchor":true},{"citing_arxiv_id":"2606.30760","citing_title":"Rich Phenomenology from Simple Ingredients: A Review of Confining Dark Sectors","ref_index":109,"is_internal_anchor":true},{"citing_arxiv_id":"2605.31527","citing_title":"Accessing Exotic Hadronic States via Charmed-Meson Femtoscopy in Relativistic Heavy-Ion Collisions","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2206.09952","citing_title":"Tachyonic AdS/QCD, Determining the Strong Running Coupling and \\beta-function in both UV and IR Regions of AdS Space","ref_index":114,"is_internal_anchor":true},{"citing_arxiv_id":"2605.01573","citing_title":"The atomic nucleus as a bound system of $3A$ quarks","ref_index":66,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/L5FJH34UEYLXW7XAG2MPERI5RK","json":"https://pith.science/pith/L5FJH34UEYLXW7XAG2MPERI5RK.json","graph_json":"https://pith.science/api/pith-number/L5FJH34UEYLXW7XAG2MPERI5RK/graph.json","events_json":"https://pith.science/api/pith-number/L5FJH34UEYLXW7XAG2MPERI5RK/events.json","paper":"https://pith.science/paper/L5FJH34U"},"agent_actions":{"view_html":"https://pith.science/pith/L5FJH34UEYLXW7XAG2MPERI5RK","download_json":"https://pith.science/pith/L5FJH34UEYLXW7XAG2MPERI5RK.json","view_paper":"https://pith.science/paper/L5FJH34U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1301.5183&json=true","fetch_graph":"https://pith.science/api/pith-number/L5FJH34UEYLXW7XAG2MPERI5RK/graph.json","fetch_events":"https://pith.science/api/pith-number/L5FJH34UEYLXW7XAG2MPERI5RK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L5FJH34UEYLXW7XAG2MPERI5RK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L5FJH34UEYLXW7XAG2MPERI5RK/action/storage_attestation","attest_author":"https://pith.science/pith/L5FJH34UEYLXW7XAG2MPERI5RK/action/author_attestation","sign_citation":"https://pith.science/pith/L5FJH34UEYLXW7XAG2MPERI5RK/action/citation_signature","submit_replication":"https://pith.science/pith/L5FJH34UEYLXW7XAG2MPERI5RK/action/replication_record"}},"created_at":"2026-05-18T03:31:44.465394+00:00","updated_at":"2026-05-18T03:31:44.465394+00:00"}