{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:24X526NY6C3KC7I2G4I6N52B5C","short_pith_number":"pith:24X526NY","schema_version":"1.0","canonical_sha256":"d72fdd79b8f0b6a17d1a3711e6f741e899eb096ea7238ae2ea10c841806418bb","source":{"kind":"arxiv","id":"2211.16178","version":2},"attestation_state":"computed","paper":{"title":"Tools for estimating fake/non-prompt lepton backgrounds with the ATLAS detector at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2022-11-29T13:11:21Z","abstract_excerpt":"Measurements and searches performed with the ATLAS detector at the CERN Large Hadron Collider often involve signatures with one or more prompt leptons. Such analyses are subject to `fake/non-prompt' lepton backgrounds, where either a hadron or a lepton from a hadron decay or an electron from a photon conversion satisfies the prompt-lepton selection criteria. These backgrounds often arise within a hadronic jet because of particle decays in the showering process, particle misidentification or particle interactions with the detector material. As it is challenging to model these processes with hig"},"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":"2211.16178","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2022-11-29T13:11:21Z","cross_cats_sorted":[],"title_canon_sha256":"510cdda392ed90517b1b341f7388041e7482b8f0c5f03ee54e4b25cf91b407b1","abstract_canon_sha256":"2cca19884b023a589eae74a98a548d79ff2eddfd3f3d631d8de59eda91334538"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:32:38.921277Z","signature_b64":"rdD/KQeoO7Zex4NWsYKCAH1dy1B0KPkkOxWxdaLMVmIp/qKCqATr4KyXDe+WjA6VGoH6uqDl8Ql6LuIfY/i+Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d72fdd79b8f0b6a17d1a3711e6f741e899eb096ea7238ae2ea10c841806418bb","last_reissued_at":"2026-07-05T09:32:38.920862Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:32:38.920862Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tools for estimating fake/non-prompt lepton backgrounds with the ATLAS detector at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2022-11-29T13:11:21Z","abstract_excerpt":"Measurements and searches performed with the ATLAS detector at the CERN Large Hadron Collider often involve signatures with one or more prompt leptons. Such analyses are subject to `fake/non-prompt' lepton backgrounds, where either a hadron or a lepton from a hadron decay or an electron from a photon conversion satisfies the prompt-lepton selection criteria. These backgrounds often arise within a hadronic jet because of particle decays in the showering process, particle misidentification or particle interactions with the detector material. As it is challenging to model these processes with hig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.16178","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/2211.16178/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":"2211.16178","created_at":"2026-07-05T09:32:38.920926+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.16178v2","created_at":"2026-07-05T09:32:38.920926+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.16178","created_at":"2026-07-05T09:32:38.920926+00:00"},{"alias_kind":"pith_short_12","alias_value":"24X526NY6C3K","created_at":"2026-07-05T09:32:38.920926+00:00"},{"alias_kind":"pith_short_16","alias_value":"24X526NY6C3KC7I2","created_at":"2026-07-05T09:32:38.920926+00:00"},{"alias_kind":"pith_short_8","alias_value":"24X526NY","created_at":"2026-07-05T09:32:38.920926+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":8,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.19016","citing_title":"Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb$^{-1}$ of data collected at $\\sqrt{s}$ = 13.6 TeV with the ATLAS dete","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2605.31205","citing_title":"Measurement of the cross-section for the production of a $W$ boson in association with $b$-jets in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":45,"is_internal_anchor":false},{"citing_arxiv_id":"2510.02857","citing_title":"Search for a resonance decaying into a scalar particle and a Higgs boson in the final state with two bottom quarks and two photons with 199 fb$^{-1}$ of data collected at $\\sqrt{s}$=13 and 13.6 TeV wi","ref_index":63,"is_internal_anchor":false},{"citing_arxiv_id":"2510.02857","citing_title":"Search for a resonance decaying into a scalar particle and a Higgs boson in the final state with two bottom quarks and two photons with 199 fb$^{-1}$ of data collected at $\\sqrt{s}$=13 and 13.6 TeV wi","ref_index":63,"is_internal_anchor":false},{"citing_arxiv_id":"2605.19016","citing_title":"Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb$^{-1}$ of data collected at $\\sqrt{s}$ = 13.6 TeV with the ATLAS dete","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2511.23091","citing_title":"Measurement of the top-quark mass using decays with a $J/\\psi$ meson at $\\sqrt{s}=$13 TeV with the ATLAS detector","ref_index":93,"is_internal_anchor":false},{"citing_arxiv_id":"2605.07585","citing_title":"Track and Vertex Reconstruction with the ATLAS Inner Detector","ref_index":94,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19495","citing_title":"Search for quantum black holes in lepton+jet final states using proton-proton collisions at $\\sqrt{s}=13.6$ TeV with the ATLAS detector","ref_index":58,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/24X526NY6C3KC7I2G4I6N52B5C","json":"https://pith.science/pith/24X526NY6C3KC7I2G4I6N52B5C.json","graph_json":"https://pith.science/api/pith-number/24X526NY6C3KC7I2G4I6N52B5C/graph.json","events_json":"https://pith.science/api/pith-number/24X526NY6C3KC7I2G4I6N52B5C/events.json","paper":"https://pith.science/paper/24X526NY"},"agent_actions":{"view_html":"https://pith.science/pith/24X526NY6C3KC7I2G4I6N52B5C","download_json":"https://pith.science/pith/24X526NY6C3KC7I2G4I6N52B5C.json","view_paper":"https://pith.science/paper/24X526NY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.16178&json=true","fetch_graph":"https://pith.science/api/pith-number/24X526NY6C3KC7I2G4I6N52B5C/graph.json","fetch_events":"https://pith.science/api/pith-number/24X526NY6C3KC7I2G4I6N52B5C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/24X526NY6C3KC7I2G4I6N52B5C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/24X526NY6C3KC7I2G4I6N52B5C/action/storage_attestation","attest_author":"https://pith.science/pith/24X526NY6C3KC7I2G4I6N52B5C/action/author_attestation","sign_citation":"https://pith.science/pith/24X526NY6C3KC7I2G4I6N52B5C/action/citation_signature","submit_replication":"https://pith.science/pith/24X526NY6C3KC7I2G4I6N52B5C/action/replication_record"}},"created_at":"2026-07-05T09:32:38.920926+00:00","updated_at":"2026-07-05T09:32:38.920926+00:00"}