{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:CQEODBMCMQHXKDQ3MW4NJARAWN","short_pith_number":"pith:CQEODBMC","schema_version":"1.0","canonical_sha256":"1408e18582640f750e1b65b8d48220b366a61c59246b97cbccd8ed378c39738d","source":{"kind":"arxiv","id":"1912.02844","version":2},"attestation_state":"computed","paper":{"title":"Measurement of the transverse momentum distribution of Drell-Yan lepton pairs in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2019-12-05T19:12:32Z","abstract_excerpt":"This paper describes precision measurements of the transverse momentum $p_\\mathrm{T}^{\\ell\\ell}$ ($\\ell=e,\\mu$) and of the angular variable $\\phi^{*}_{\\eta}$ distributions of Drell-Yan lepton pairs in a mass range of 66-116 GeV. The analysis uses data from 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\\sqrt{s}=13$ TeV collected by the ATLAS experiment at the LHC in 2015 and 2016. Measurements in electron-pair and muon-pair final states are performed in the same fiducial volumes, corrected for detector effects, and combined. Compared to previous measurements in proto"},"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":"1912.02844","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-12-05T19:12:32Z","cross_cats_sorted":[],"title_canon_sha256":"cde8acdf70551be07e02c18cb07244f571aa04020eea2f90b221ed49de85ebd1","abstract_canon_sha256":"bdbcc0569733316cce862d106dcc5148da3c8b415fdd696ef18bf578c4ce4e77"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:59:27.228288Z","signature_b64":"G7m6LxU27MBqmdkEJA81zvbb85d1mOfL9Qm+e4fE3VHydNBkIVmQNs1y4a8t8z8fwyIOYFboRasi49+XsLbHDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1408e18582640f750e1b65b8d48220b366a61c59246b97cbccd8ed378c39738d","last_reissued_at":"2026-07-05T01:59:27.227871Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:59:27.227871Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the transverse momentum distribution of Drell-Yan lepton pairs in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2019-12-05T19:12:32Z","abstract_excerpt":"This paper describes precision measurements of the transverse momentum $p_\\mathrm{T}^{\\ell\\ell}$ ($\\ell=e,\\mu$) and of the angular variable $\\phi^{*}_{\\eta}$ distributions of Drell-Yan lepton pairs in a mass range of 66-116 GeV. The analysis uses data from 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\\sqrt{s}=13$ TeV collected by the ATLAS experiment at the LHC in 2015 and 2016. Measurements in electron-pair and muon-pair final states are performed in the same fiducial volumes, corrected for detector effects, and combined. Compared to previous measurements in proto"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1912.02844","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/1912.02844/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":"1912.02844","created_at":"2026-07-05T01:59:27.227926+00:00"},{"alias_kind":"arxiv_version","alias_value":"1912.02844v2","created_at":"2026-07-05T01:59:27.227926+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1912.02844","created_at":"2026-07-05T01:59:27.227926+00:00"},{"alias_kind":"pith_short_12","alias_value":"CQEODBMCMQHX","created_at":"2026-07-05T01:59:27.227926+00:00"},{"alias_kind":"pith_short_16","alias_value":"CQEODBMCMQHXKDQ3","created_at":"2026-07-05T01:59:27.227926+00:00"},{"alias_kind":"pith_short_8","alias_value":"CQEODBMC","created_at":"2026-07-05T01:59:27.227926+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2212.09379","citing_title":"Luminosity determination in $pp$ collisions at $\\sqrt{s}=13$ TeV using the ATLAS detector at the LHC","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2605.10287","citing_title":"Phenomenology of electroweak spin-1 resonances","ref_index":85,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12706","citing_title":"Measurement of the $W$-boson production cross-sections in $pp$ collisions at $\\sqrt{s}$ = 13 TeV in the forward region","ref_index":24,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CQEODBMCMQHXKDQ3MW4NJARAWN","json":"https://pith.science/pith/CQEODBMCMQHXKDQ3MW4NJARAWN.json","graph_json":"https://pith.science/api/pith-number/CQEODBMCMQHXKDQ3MW4NJARAWN/graph.json","events_json":"https://pith.science/api/pith-number/CQEODBMCMQHXKDQ3MW4NJARAWN/events.json","paper":"https://pith.science/paper/CQEODBMC"},"agent_actions":{"view_html":"https://pith.science/pith/CQEODBMCMQHXKDQ3MW4NJARAWN","download_json":"https://pith.science/pith/CQEODBMCMQHXKDQ3MW4NJARAWN.json","view_paper":"https://pith.science/paper/CQEODBMC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1912.02844&json=true","fetch_graph":"https://pith.science/api/pith-number/CQEODBMCMQHXKDQ3MW4NJARAWN/graph.json","fetch_events":"https://pith.science/api/pith-number/CQEODBMCMQHXKDQ3MW4NJARAWN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CQEODBMCMQHXKDQ3MW4NJARAWN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CQEODBMCMQHXKDQ3MW4NJARAWN/action/storage_attestation","attest_author":"https://pith.science/pith/CQEODBMCMQHXKDQ3MW4NJARAWN/action/author_attestation","sign_citation":"https://pith.science/pith/CQEODBMCMQHXKDQ3MW4NJARAWN/action/citation_signature","submit_replication":"https://pith.science/pith/CQEODBMCMQHXKDQ3MW4NJARAWN/action/replication_record"}},"created_at":"2026-07-05T01:59:27.227926+00:00","updated_at":"2026-07-05T01:59:27.227926+00:00"}