{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:QLWIUUJSML5LYW5HCJDXEPRFTH","short_pith_number":"pith:QLWIUUJS","schema_version":"1.0","canonical_sha256":"82ec8a513262fabc5ba71247723e2599ea81fef9649a6e2fc96bc61c77b64a3d","source":{"kind":"arxiv","id":"hep-ph/9407339","version":2},"attestation_state":"computed","paper":{"title":"Rigorous QCD Analysis of Inclusive Annihilation and Production of Heavy Quarkonium","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Eric Braaten, Geoffrey T. Bodwin, G. Peter Lepage","submitted_at":"1994-07-20T22:11:47Z","abstract_excerpt":"A rigorous QCD analysis of the inclusive annihilation decay rates of heavy quarkonium states is presented. The effective-field-theory framework of nonrelativistic QCD is used to separate the short-distance scale of annihilation, which is set by the heavy quark mass $M$, from the longer-distance scales associated with quarkonium structure. The annihilation decay rates are expressed in terms of nonperturbative matrix elements of 4-fermion operators in nonrelativistic QCD, with coefficients that can be computed using perturbation theory in the coupling constant $\\alpha_s(M)$. The matrix elements "},"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":"hep-ph/9407339","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-07-20T22:11:47Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"48c53ffe333b59d771714a3a4f8da3cc4a04bdb68b293217e8fad664dd39be19","abstract_canon_sha256":"3f6ebb980f69c2074b8ba1cb3d2a82cd6f3244396e9fa40dd860b1ec9c652e3d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:37:13.170736Z","signature_b64":"Ez3d3ygHTxFahV73LMUogzOt6j54hSUy2FnJd14JZF05Y5lVr59tfAvbX9ov8qdna7CLQFqEN7psRTzx0j+YDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"82ec8a513262fabc5ba71247723e2599ea81fef9649a6e2fc96bc61c77b64a3d","last_reissued_at":"2026-05-18T02:37:13.170284Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:37:13.170284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Rigorous QCD Analysis of Inclusive Annihilation and Production of Heavy Quarkonium","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Eric Braaten, Geoffrey T. Bodwin, G. Peter Lepage","submitted_at":"1994-07-20T22:11:47Z","abstract_excerpt":"A rigorous QCD analysis of the inclusive annihilation decay rates of heavy quarkonium states is presented. The effective-field-theory framework of nonrelativistic QCD is used to separate the short-distance scale of annihilation, which is set by the heavy quark mass $M$, from the longer-distance scales associated with quarkonium structure. The annihilation decay rates are expressed in terms of nonperturbative matrix elements of 4-fermion operators in nonrelativistic QCD, with coefficients that can be computed using perturbation theory in the coupling constant $\\alpha_s(M)$. The matrix elements "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9407339","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":""},"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":"hep-ph/9407339","created_at":"2026-05-18T02:37:13.170352+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9407339v2","created_at":"2026-05-18T02:37:13.170352+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9407339","created_at":"2026-05-18T02:37:13.170352+00:00"},{"alias_kind":"pith_short_12","alias_value":"QLWIUUJSML5L","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"QLWIUUJSML5LYW5H","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"QLWIUUJS","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":18,"internal_anchor_count":10,"sample":[{"citing_arxiv_id":"1906.10049","citing_title":"Prompt ${J/\\psi}$-pair production at the LHC: impact of loop-induced contributions and of the colour-octet mechanism","ref_index":52,"is_internal_anchor":true},{"citing_arxiv_id":"1907.04419","citing_title":"Toward an effective theory of quarkonium production in nuclear matter","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2605.22500","citing_title":"Two photon decay width of the fully charmed tetraquarks: revisiting prospects for ultraperipheral collisions","ref_index":30,"is_internal_anchor":true},{"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":16,"is_internal_anchor":true},{"citing_arxiv_id":"2605.19300","citing_title":"The twist-3 gluon contribution to $A_N$ in $J/\\psi$ production in $pp$ collisions","ref_index":45,"is_internal_anchor":true},{"citing_arxiv_id":"2506.17454","citing_title":"Nuclear Cold QCD: Review and Future Strategy","ref_index":69,"is_internal_anchor":true},{"citing_arxiv_id":"2510.11809","citing_title":"Modeling the TMD shape function in $J/\\psi$ electroproduction","ref_index":4,"is_internal_anchor":true},{"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":16,"is_internal_anchor":true},{"citing_arxiv_id":"2602.12611","citing_title":"Resummation of threshold double logarithms in quarkonium fragmentation functions","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13977","citing_title":"A Phenomenological Model of Mesons for Charged Current Weak Decays","ref_index":113,"is_internal_anchor":true},{"citing_arxiv_id":"2605.01539","citing_title":"Multimodal Fragmentation of All-Heavy Pentaquarks: Uncertainty-Aware Predictions for Hadron Colliders","ref_index":124,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21838","citing_title":"True Leptonium ($l^+ l^-$) Production in UPC Triphoton Interaction","ref_index":27,"is_internal_anchor":false},{"citing_arxiv_id":"2604.11646","citing_title":"All-charm tetraquarks at hadron colliders: A high-precision fragmentation perspective","ref_index":146,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12603","citing_title":"Open-flavor threshold effects on quarkonium spectrum in the BOEFT","ref_index":91,"is_internal_anchor":false},{"citing_arxiv_id":"2604.11123","citing_title":"Measurement of inclusive production of charmonium states in $b$-hadron decays via their decay into $\\phi \\phi$","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07968","citing_title":"Multiplicity dependence of prompt and non-prompt J/$\\psi$ production at midrapidity in pp collisions at $\\sqrt{s} = 13$ TeV","ref_index":2,"is_internal_anchor":false},{"citing_arxiv_id":"2604.17726","citing_title":"Searching for dark photons in $J/\\psi$ decays","ref_index":10,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15256","citing_title":"Charmonium radiative transitions to dileptons from lattice QCD: The case of $h_c \\to \\eta_c \\ell^+\\ell^-$ and $\\chi_{c1} \\to J/\\psi\\,\\ell^+\\ell^-$","ref_index":1,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QLWIUUJSML5LYW5HCJDXEPRFTH","json":"https://pith.science/pith/QLWIUUJSML5LYW5HCJDXEPRFTH.json","graph_json":"https://pith.science/api/pith-number/QLWIUUJSML5LYW5HCJDXEPRFTH/graph.json","events_json":"https://pith.science/api/pith-number/QLWIUUJSML5LYW5HCJDXEPRFTH/events.json","paper":"https://pith.science/paper/QLWIUUJS"},"agent_actions":{"view_html":"https://pith.science/pith/QLWIUUJSML5LYW5HCJDXEPRFTH","download_json":"https://pith.science/pith/QLWIUUJSML5LYW5HCJDXEPRFTH.json","view_paper":"https://pith.science/paper/QLWIUUJS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9407339&json=true","fetch_graph":"https://pith.science/api/pith-number/QLWIUUJSML5LYW5HCJDXEPRFTH/graph.json","fetch_events":"https://pith.science/api/pith-number/QLWIUUJSML5LYW5HCJDXEPRFTH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QLWIUUJSML5LYW5HCJDXEPRFTH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QLWIUUJSML5LYW5HCJDXEPRFTH/action/storage_attestation","attest_author":"https://pith.science/pith/QLWIUUJSML5LYW5HCJDXEPRFTH/action/author_attestation","sign_citation":"https://pith.science/pith/QLWIUUJSML5LYW5HCJDXEPRFTH/action/citation_signature","submit_replication":"https://pith.science/pith/QLWIUUJSML5LYW5HCJDXEPRFTH/action/replication_record"}},"created_at":"2026-05-18T02:37:13.170352+00:00","updated_at":"2026-05-18T02:37:13.170352+00:00"}