{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:OL7B4ZEUBDDMWNCTUGDWRDV4CP","short_pith_number":"pith:OL7B4ZEU","schema_version":"1.0","canonical_sha256":"72fe1e649408c6cb3453a187688ebc13f81d2f32ee618bdb8b61db5a463f92f9","source":{"kind":"arxiv","id":"1612.03016","version":2},"attestation_state":"computed","paper":{"title":"Precision measurement and interpretation of inclusive $W^+$, $W^-$ and $Z/\\gamma^*$ production cross sections with the ATLAS detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2016-12-09T13:38:48Z","abstract_excerpt":"High-precision measurements by the ATLAS Collaboration are presented of inclusive $W^+\\to\\ell^+\\nu$, $W^-\\to\\ell^-\\bar{\\nu}$ and $Z/\\gamma^*\\to\\ell\\ell$ ($\\ell=e,\\mu$) Drell-Yan production cross sections at the LHC. The data were collected in proton-proton collisions at $\\sqrt{s} = 7$ TeV with an integrated luminosity of 4.6 fb$^{-1}$. Differential $W^+$ and $W^-$ cross sections are measured in a lepton pseudorapidity range $|\\eta_{\\ell}| = 2.5$. Differential $Z/\\gamma^*$ cross sections are measured as a function of the absolute dilepton rapidity, for $|y_{\\ell\\ell}| < 3.6$, for three interval"},"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":"1612.03016","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2016-12-09T13:38:48Z","cross_cats_sorted":[],"title_canon_sha256":"54d134327deaa11e9620a8268d380caa7e7199dc359606c763f862a9beea5c3a","abstract_canon_sha256":"e759a8548dd2dd053584cfd201435b1fa6a72c797f1f757f2709ef705d249898"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:42:46.347540Z","signature_b64":"+Urt2bRXNLnJtHUvDgTZdtyGTU9L3TMBg1dQTI17lQI7NNoVzMG9GUhVFJcaDGh3tc+axlL2hWGGKzt1ycOCBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"72fe1e649408c6cb3453a187688ebc13f81d2f32ee618bdb8b61db5a463f92f9","last_reissued_at":"2026-05-18T00:42:46.346877Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:42:46.346877Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Precision measurement and interpretation of inclusive $W^+$, $W^-$ and $Z/\\gamma^*$ production cross sections with the ATLAS detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2016-12-09T13:38:48Z","abstract_excerpt":"High-precision measurements by the ATLAS Collaboration are presented of inclusive $W^+\\to\\ell^+\\nu$, $W^-\\to\\ell^-\\bar{\\nu}$ and $Z/\\gamma^*\\to\\ell\\ell$ ($\\ell=e,\\mu$) Drell-Yan production cross sections at the LHC. The data were collected in proton-proton collisions at $\\sqrt{s} = 7$ TeV with an integrated luminosity of 4.6 fb$^{-1}$. Differential $W^+$ and $W^-$ cross sections are measured in a lepton pseudorapidity range $|\\eta_{\\ell}| = 2.5$. Differential $Z/\\gamma^*$ cross sections are measured as a function of the absolute dilepton rapidity, for $|y_{\\ell\\ell}| < 3.6$, for three interval"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.03016","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":"1612.03016","created_at":"2026-05-18T00:42:46.346976+00:00"},{"alias_kind":"arxiv_version","alias_value":"1612.03016v2","created_at":"2026-05-18T00:42:46.346976+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.03016","created_at":"2026-05-18T00:42:46.346976+00:00"},{"alias_kind":"pith_short_12","alias_value":"OL7B4ZEUBDDM","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_16","alias_value":"OL7B4ZEUBDDMWNCT","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_8","alias_value":"OL7B4ZEU","created_at":"2026-05-18T12:30:36.002864+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.19918","citing_title":"Redetermination of proton sea distributions","ref_index":27,"is_internal_anchor":true},{"citing_arxiv_id":"2604.21670","citing_title":"Effective field theory interpretation of ATLAS measurements involving the Higgs boson, electroweak bosons and the top quark","ref_index":30,"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":27,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12593","citing_title":"Precision measurement of the muon charge asymmetry from $W$-boson decays 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/OL7B4ZEUBDDMWNCTUGDWRDV4CP","json":"https://pith.science/pith/OL7B4ZEUBDDMWNCTUGDWRDV4CP.json","graph_json":"https://pith.science/api/pith-number/OL7B4ZEUBDDMWNCTUGDWRDV4CP/graph.json","events_json":"https://pith.science/api/pith-number/OL7B4ZEUBDDMWNCTUGDWRDV4CP/events.json","paper":"https://pith.science/paper/OL7B4ZEU"},"agent_actions":{"view_html":"https://pith.science/pith/OL7B4ZEUBDDMWNCTUGDWRDV4CP","download_json":"https://pith.science/pith/OL7B4ZEUBDDMWNCTUGDWRDV4CP.json","view_paper":"https://pith.science/paper/OL7B4ZEU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1612.03016&json=true","fetch_graph":"https://pith.science/api/pith-number/OL7B4ZEUBDDMWNCTUGDWRDV4CP/graph.json","fetch_events":"https://pith.science/api/pith-number/OL7B4ZEUBDDMWNCTUGDWRDV4CP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OL7B4ZEUBDDMWNCTUGDWRDV4CP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OL7B4ZEUBDDMWNCTUGDWRDV4CP/action/storage_attestation","attest_author":"https://pith.science/pith/OL7B4ZEUBDDMWNCTUGDWRDV4CP/action/author_attestation","sign_citation":"https://pith.science/pith/OL7B4ZEUBDDMWNCTUGDWRDV4CP/action/citation_signature","submit_replication":"https://pith.science/pith/OL7B4ZEUBDDMWNCTUGDWRDV4CP/action/replication_record"}},"created_at":"2026-05-18T00:42:46.346976+00:00","updated_at":"2026-05-18T00:42:46.346976+00:00"}