{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:4KDSA7QICMUN6GAUFUKDXYUCEJ","short_pith_number":"pith:4KDSA7QI","schema_version":"1.0","canonical_sha256":"e287207e081328df18142d143be2822248f5d3c2439d36bca7b48fe0a7a9078e","source":{"kind":"arxiv","id":"1304.7498","version":2},"attestation_state":"computed","paper":{"title":"Measurement of the ratio of the inclusive 3-jet cross section to the inclusive 2-jet cross section in pp collisions at sqrt(s) = 7 TeV and first determination of the strong coupling constant in the TeV range","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2013-04-28T18:54:47Z","abstract_excerpt":"A measurement is presented of the ratio of the inclusive 3-jet cross section to the inclusive 2-jet cross section as a function of the average transverse momentum, <pT[1,2]>, of the two leading jets in the event. The data sample was collected during 2011 at a proton-proton centre-of-mass energy of 7 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 5.0 inverse femtobarns. The strong coupling constant at the scale of the Z boson mass is determined to be alphaS[MZ] = 0.1148 +/- 0.0014 (exp.) +/- 0.0018 (PDF) +/- 0.0050 (theory), by comparing the ratio in the rang"},"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":"1304.7498","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2013-04-28T18:54:47Z","cross_cats_sorted":[],"title_canon_sha256":"ab7d218982b21fed88082399fc058e3ee7988a7689f58e574ff2c0bc57f1c0fb","abstract_canon_sha256":"b498908f949e73451f524db2ab23a4ebb2676c44e4671b545390a3e8fe66a363"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:05:54.628623Z","signature_b64":"JZZSUgqljgaibHT/AvmHvU1eqE8k54Jfp9ezHekFyCJosMZHzH1Tw/B9GeUqeTEc8R7TWO7ht5AAFTUt3ju5Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e287207e081328df18142d143be2822248f5d3c2439d36bca7b48fe0a7a9078e","last_reissued_at":"2026-05-18T03:05:54.628002Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:05:54.628002Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the ratio of the inclusive 3-jet cross section to the inclusive 2-jet cross section in pp collisions at sqrt(s) = 7 TeV and first determination of the strong coupling constant in the TeV range","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2013-04-28T18:54:47Z","abstract_excerpt":"A measurement is presented of the ratio of the inclusive 3-jet cross section to the inclusive 2-jet cross section as a function of the average transverse momentum, <pT[1,2]>, of the two leading jets in the event. The data sample was collected during 2011 at a proton-proton centre-of-mass energy of 7 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 5.0 inverse femtobarns. The strong coupling constant at the scale of the Z boson mass is determined to be alphaS[MZ] = 0.1148 +/- 0.0014 (exp.) +/- 0.0018 (PDF) +/- 0.0050 (theory), by comparing the ratio in the rang"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.7498","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":"1304.7498","created_at":"2026-05-18T03:05:54.628093+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.7498v2","created_at":"2026-05-18T03:05:54.628093+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.7498","created_at":"2026-05-18T03:05:54.628093+00:00"},{"alias_kind":"pith_short_12","alias_value":"4KDSA7QICMUN","created_at":"2026-05-18T12:27:34.582898+00:00"},{"alias_kind":"pith_short_16","alias_value":"4KDSA7QICMUN6GAU","created_at":"2026-05-18T12:27:34.582898+00:00"},{"alias_kind":"pith_short_8","alias_value":"4KDSA7QI","created_at":"2026-05-18T12:27:34.582898+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.12250","citing_title":"Anisotropic jet broadening and jet shape","ref_index":9,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4KDSA7QICMUN6GAUFUKDXYUCEJ","json":"https://pith.science/pith/4KDSA7QICMUN6GAUFUKDXYUCEJ.json","graph_json":"https://pith.science/api/pith-number/4KDSA7QICMUN6GAUFUKDXYUCEJ/graph.json","events_json":"https://pith.science/api/pith-number/4KDSA7QICMUN6GAUFUKDXYUCEJ/events.json","paper":"https://pith.science/paper/4KDSA7QI"},"agent_actions":{"view_html":"https://pith.science/pith/4KDSA7QICMUN6GAUFUKDXYUCEJ","download_json":"https://pith.science/pith/4KDSA7QICMUN6GAUFUKDXYUCEJ.json","view_paper":"https://pith.science/paper/4KDSA7QI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.7498&json=true","fetch_graph":"https://pith.science/api/pith-number/4KDSA7QICMUN6GAUFUKDXYUCEJ/graph.json","fetch_events":"https://pith.science/api/pith-number/4KDSA7QICMUN6GAUFUKDXYUCEJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4KDSA7QICMUN6GAUFUKDXYUCEJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4KDSA7QICMUN6GAUFUKDXYUCEJ/action/storage_attestation","attest_author":"https://pith.science/pith/4KDSA7QICMUN6GAUFUKDXYUCEJ/action/author_attestation","sign_citation":"https://pith.science/pith/4KDSA7QICMUN6GAUFUKDXYUCEJ/action/citation_signature","submit_replication":"https://pith.science/pith/4KDSA7QICMUN6GAUFUKDXYUCEJ/action/replication_record"}},"created_at":"2026-05-18T03:05:54.628093+00:00","updated_at":"2026-05-18T03:05:54.628093+00:00"}