{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:24JV42S6ZRVEFSFQUMFD6SRHCT","short_pith_number":"pith:24JV42S6","schema_version":"1.0","canonical_sha256":"d7135e6a5ecc6a42c8b0a30a3f4a2714e3187451c36ac4b72012ef91acc2e8db","source":{"kind":"arxiv","id":"1512.06212","version":2},"attestation_state":"computed","paper":{"title":"Measurement of the inclusive jet cross section in pp collisions at sqrt(s) = 2.76 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2015-12-19T09:23:58Z","abstract_excerpt":"The double-differential inclusive jet cross section is measured as a function of jet transverse momentum pT and absolute rapidity y, using proton-proton collision data collected with the CMS experiment at the LHC, at a center-of-mass energy of sqrt(s) = 2.76 TeV and corresponding to an integrated luminosity of 5.43 inverse picoboarns. Jets are reconstructed within the pT range of 74 to 592 GeV and the rapidity range |y| < 3.0. The reconstructed jet spectrum is corrected for detector resolution. The measurements are compared to the theoretical prediction at next-to-leading-order QCD using diffe"},"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":"1512.06212","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2015-12-19T09:23:58Z","cross_cats_sorted":[],"title_canon_sha256":"9d81b5750d62bd21ca349ae5867b8cebf01da3b733974efd95f5a13eb3f0d9a6","abstract_canon_sha256":"c1c1e9013b76eb977bcddc28f080ee94333d1e4f5b7aff8c09947282ca3f7d11"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:14:01.460567Z","signature_b64":"Zm/9RaJ8Hi0E7uTpTfwEq/8+siUE9nAE5DKXIIgthp0dVgPfvthJ08LodFU+sZqHcepzmNDHqzQ4jNzhVNGcDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d7135e6a5ecc6a42c8b0a30a3f4a2714e3187451c36ac4b72012ef91acc2e8db","last_reissued_at":"2026-05-18T01:14:01.459972Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:14:01.459972Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the inclusive jet cross section in pp collisions at sqrt(s) = 2.76 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2015-12-19T09:23:58Z","abstract_excerpt":"The double-differential inclusive jet cross section is measured as a function of jet transverse momentum pT and absolute rapidity y, using proton-proton collision data collected with the CMS experiment at the LHC, at a center-of-mass energy of sqrt(s) = 2.76 TeV and corresponding to an integrated luminosity of 5.43 inverse picoboarns. Jets are reconstructed within the pT range of 74 to 592 GeV and the rapidity range |y| < 3.0. The reconstructed jet spectrum is corrected for detector resolution. The measurements are compared to the theoretical prediction at next-to-leading-order QCD using diffe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.06212","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":"1512.06212","created_at":"2026-05-18T01:14:01.460089+00:00"},{"alias_kind":"arxiv_version","alias_value":"1512.06212v2","created_at":"2026-05-18T01:14:01.460089+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.06212","created_at":"2026-05-18T01:14:01.460089+00:00"},{"alias_kind":"pith_short_12","alias_value":"24JV42S6ZRVE","created_at":"2026-05-18T12:28:59.999130+00:00"},{"alias_kind":"pith_short_16","alias_value":"24JV42S6ZRVEFSFQ","created_at":"2026-05-18T12:28:59.999130+00:00"},{"alias_kind":"pith_short_8","alias_value":"24JV42S6","created_at":"2026-05-18T12:28:59.999130+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.16665","citing_title":"Determination of the strong coupling and its running from measurements of inclusive jet production","ref_index":1,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/24JV42S6ZRVEFSFQUMFD6SRHCT","json":"https://pith.science/pith/24JV42S6ZRVEFSFQUMFD6SRHCT.json","graph_json":"https://pith.science/api/pith-number/24JV42S6ZRVEFSFQUMFD6SRHCT/graph.json","events_json":"https://pith.science/api/pith-number/24JV42S6ZRVEFSFQUMFD6SRHCT/events.json","paper":"https://pith.science/paper/24JV42S6"},"agent_actions":{"view_html":"https://pith.science/pith/24JV42S6ZRVEFSFQUMFD6SRHCT","download_json":"https://pith.science/pith/24JV42S6ZRVEFSFQUMFD6SRHCT.json","view_paper":"https://pith.science/paper/24JV42S6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1512.06212&json=true","fetch_graph":"https://pith.science/api/pith-number/24JV42S6ZRVEFSFQUMFD6SRHCT/graph.json","fetch_events":"https://pith.science/api/pith-number/24JV42S6ZRVEFSFQUMFD6SRHCT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/24JV42S6ZRVEFSFQUMFD6SRHCT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/24JV42S6ZRVEFSFQUMFD6SRHCT/action/storage_attestation","attest_author":"https://pith.science/pith/24JV42S6ZRVEFSFQUMFD6SRHCT/action/author_attestation","sign_citation":"https://pith.science/pith/24JV42S6ZRVEFSFQUMFD6SRHCT/action/citation_signature","submit_replication":"https://pith.science/pith/24JV42S6ZRVEFSFQUMFD6SRHCT/action/replication_record"}},"created_at":"2026-05-18T01:14:01.460089+00:00","updated_at":"2026-05-18T01:14:01.460089+00:00"}