{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:YIQHO7WWSAQZT2KHELIODERRGK","short_pith_number":"pith:YIQHO7WW","schema_version":"1.0","canonical_sha256":"c220777ed6902199e94722d0e19231329ba2f1391bf86fd3196472f010153f6a","source":{"kind":"arxiv","id":"2505.03869","version":2},"attestation_state":"computed","paper":{"title":"Toponium physics at the Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Benjamin Fuks","submitted_at":"2025-05-06T18:00:00Z","abstract_excerpt":"We examine toponium formation effects in top-antitop pair production at the LHC, focusing on the near-threshold region where non-relativistic corrections are relevant. We discuss their modelling using non-relativistic QCD Green's functions, and show that predictions reproduce features expected from bound-state dynamics, in contrast to pseudo-scalar toy models."},"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":"2505.03869","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-06T18:00:00Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"881d24721fe870a0b9d352422e81b7be5559fdbbc08375e7ee4fa691c099f333","abstract_canon_sha256":"ab42081ce8490b2143c6665942d4bcbcb416fdf5b8b731be12ba3352b4261cd8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:01:36.260279Z","signature_b64":"2MW7RM/Hc7EkoELVRLoxjI8Z/xmZMK4GsBnj80yCVAZuedncqnyXCdpXGryHtxXNp9xLNfDce5UJLpZExBVaBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c220777ed6902199e94722d0e19231329ba2f1391bf86fd3196472f010153f6a","last_reissued_at":"2026-07-05T11:01:36.259808Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:01:36.259808Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Toponium physics at the Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Benjamin Fuks","submitted_at":"2025-05-06T18:00:00Z","abstract_excerpt":"We examine toponium formation effects in top-antitop pair production at the LHC, focusing on the near-threshold region where non-relativistic corrections are relevant. We discuss their modelling using non-relativistic QCD Green's functions, and show that predictions reproduce features expected from bound-state dynamics, in contrast to pseudo-scalar toy models."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.03869","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/2505.03869/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":"2505.03869","created_at":"2026-07-05T11:01:36.259872+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.03869v2","created_at":"2026-07-05T11:01:36.259872+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.03869","created_at":"2026-07-05T11:01:36.259872+00:00"},{"alias_kind":"pith_short_12","alias_value":"YIQHO7WWSAQZ","created_at":"2026-07-05T11:01:36.259872+00:00"},{"alias_kind":"pith_short_16","alias_value":"YIQHO7WWSAQZT2KH","created_at":"2026-07-05T11:01:36.259872+00:00"},{"alias_kind":"pith_short_8","alias_value":"YIQHO7WW","created_at":"2026-07-05T11:01:36.259872+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2509.03596","citing_title":"Prospects for toponium formation at the LHC in the single-lepton mode","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2510.16828","citing_title":"Possible mixing between elementary and bound state fields in the $t\\bar{t}$ production excess at the LHC","ref_index":30,"is_internal_anchor":false},{"citing_arxiv_id":"2511.10053","citing_title":"Masses of Purely Top-Quark Bound States: Toponium and the Triply-Top Baryon","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00748","citing_title":"Phenomenology of Hypothetical Single-Top Hadronic States","ref_index":61,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YIQHO7WWSAQZT2KHELIODERRGK","json":"https://pith.science/pith/YIQHO7WWSAQZT2KHELIODERRGK.json","graph_json":"https://pith.science/api/pith-number/YIQHO7WWSAQZT2KHELIODERRGK/graph.json","events_json":"https://pith.science/api/pith-number/YIQHO7WWSAQZT2KHELIODERRGK/events.json","paper":"https://pith.science/paper/YIQHO7WW"},"agent_actions":{"view_html":"https://pith.science/pith/YIQHO7WWSAQZT2KHELIODERRGK","download_json":"https://pith.science/pith/YIQHO7WWSAQZT2KHELIODERRGK.json","view_paper":"https://pith.science/paper/YIQHO7WW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.03869&json=true","fetch_graph":"https://pith.science/api/pith-number/YIQHO7WWSAQZT2KHELIODERRGK/graph.json","fetch_events":"https://pith.science/api/pith-number/YIQHO7WWSAQZT2KHELIODERRGK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YIQHO7WWSAQZT2KHELIODERRGK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YIQHO7WWSAQZT2KHELIODERRGK/action/storage_attestation","attest_author":"https://pith.science/pith/YIQHO7WWSAQZT2KHELIODERRGK/action/author_attestation","sign_citation":"https://pith.science/pith/YIQHO7WWSAQZT2KHELIODERRGK/action/citation_signature","submit_replication":"https://pith.science/pith/YIQHO7WWSAQZT2KHELIODERRGK/action/replication_record"}},"created_at":"2026-07-05T11:01:36.259872+00:00","updated_at":"2026-07-05T11:01:36.259872+00:00"}