{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:MGWWS6NKLOABV5O4PSDX746WT7","short_pith_number":"pith:MGWWS6NK","schema_version":"1.0","canonical_sha256":"61ad6979aa5b801af5dc7c877ff3d69fc18f8a9163c60b40a479edf350535bbb","source":{"kind":"arxiv","id":"1303.5900","version":2},"attestation_state":"computed","paper":{"title":"Measurement of the Y(1S), Y(2S), and Y(3S) cross sections in pp collisions at sqrt(s) = 7 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2013-03-24T00:05:58Z","abstract_excerpt":"The Upsilon(1S), Upsilon(2S), and Upsilon(3S) production cross sections are measured using a data sample corresponding to an integrated luminosity of 35.8 +/-1.4 inverse picobarns of proton-proton collisions at sqrt(s) = 7 TeV, collected with the CMS detector at the LHC. The Upsilon resonances are identified through their decays to dimuons. Integrated over the Upsilon transverse momentum range pt[Upsilon] < 50 GeV and rapidity range abs(y[Upsilon]) < 2.4, and assuming unpolarized Upsilon production, the products of the Upsilon production cross sections and dimuon branching fractions are sigma("},"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":"1303.5900","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2013-03-24T00:05:58Z","cross_cats_sorted":[],"title_canon_sha256":"60d208c311b3f8e506c53470506fb9b80fa045091fbe893366cb89c711993cb4","abstract_canon_sha256":"1a59c5e7c56221e00d1770ef70c11faef4572e7396b078b05ed8766ffd4b0ffd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:07:34.302125Z","signature_b64":"/IwmQEiuGiHvJBmKg5t1+iI8JD1yQ7n4Mk0cG4TBu5a9Rmh7Llbz/oVP73S0To2MLo5VKbrXqNiImr5jDv6RAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"61ad6979aa5b801af5dc7c877ff3d69fc18f8a9163c60b40a479edf350535bbb","last_reissued_at":"2026-05-18T03:07:34.301668Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:07:34.301668Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the Y(1S), Y(2S), and Y(3S) cross sections in pp collisions at sqrt(s) = 7 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2013-03-24T00:05:58Z","abstract_excerpt":"The Upsilon(1S), Upsilon(2S), and Upsilon(3S) production cross sections are measured using a data sample corresponding to an integrated luminosity of 35.8 +/-1.4 inverse picobarns of proton-proton collisions at sqrt(s) = 7 TeV, collected with the CMS detector at the LHC. The Upsilon resonances are identified through their decays to dimuons. Integrated over the Upsilon transverse momentum range pt[Upsilon] < 50 GeV and rapidity range abs(y[Upsilon]) < 2.4, and assuming unpolarized Upsilon production, the products of the Upsilon production cross sections and dimuon branching fractions are sigma("},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.5900","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":"1303.5900","created_at":"2026-05-18T03:07:34.301747+00:00"},{"alias_kind":"arxiv_version","alias_value":"1303.5900v2","created_at":"2026-05-18T03:07:34.301747+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.5900","created_at":"2026-05-18T03:07:34.301747+00:00"},{"alias_kind":"pith_short_12","alias_value":"MGWWS6NKLOAB","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_16","alias_value":"MGWWS6NKLOABV5O4","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_8","alias_value":"MGWWS6NK","created_at":"2026-05-18T12:27:52.871228+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.04558","citing_title":"Effects of event-by-event hydrodynamic fluctuations on bottomonium dynamics in Pb--Pb collisions at $\\sqrt{s_{NN}} = 5.02$ TeV","ref_index":31,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MGWWS6NKLOABV5O4PSDX746WT7","json":"https://pith.science/pith/MGWWS6NKLOABV5O4PSDX746WT7.json","graph_json":"https://pith.science/api/pith-number/MGWWS6NKLOABV5O4PSDX746WT7/graph.json","events_json":"https://pith.science/api/pith-number/MGWWS6NKLOABV5O4PSDX746WT7/events.json","paper":"https://pith.science/paper/MGWWS6NK"},"agent_actions":{"view_html":"https://pith.science/pith/MGWWS6NKLOABV5O4PSDX746WT7","download_json":"https://pith.science/pith/MGWWS6NKLOABV5O4PSDX746WT7.json","view_paper":"https://pith.science/paper/MGWWS6NK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1303.5900&json=true","fetch_graph":"https://pith.science/api/pith-number/MGWWS6NKLOABV5O4PSDX746WT7/graph.json","fetch_events":"https://pith.science/api/pith-number/MGWWS6NKLOABV5O4PSDX746WT7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MGWWS6NKLOABV5O4PSDX746WT7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MGWWS6NKLOABV5O4PSDX746WT7/action/storage_attestation","attest_author":"https://pith.science/pith/MGWWS6NKLOABV5O4PSDX746WT7/action/author_attestation","sign_citation":"https://pith.science/pith/MGWWS6NKLOABV5O4PSDX746WT7/action/citation_signature","submit_replication":"https://pith.science/pith/MGWWS6NKLOABV5O4PSDX746WT7/action/replication_record"}},"created_at":"2026-05-18T03:07:34.301747+00:00","updated_at":"2026-05-18T03:07:34.301747+00:00"}