{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:XCHWEQAPLDEVOYQLY7TWSNX7W6","short_pith_number":"pith:XCHWEQAP","schema_version":"1.0","canonical_sha256":"b88f62400f58c957620bc7e76936ffb7a899e7b8394f9cb0cb8dbfc27eb0bdfc","source":{"kind":"arxiv","id":"2402.05858","version":2},"attestation_state":"computed","paper":{"title":"The performance of missing transverse momentum reconstruction and its significance with the ATLAS detector using 140 fb$^{-1}$ of $\\sqrt{s}=13$ TeV $pp$ collisions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2024-02-08T17:42:34Z","abstract_excerpt":"This paper presents the reconstruction of missing transverse momentum ($p_{\\text{T}}^{\\text{miss}}$) in proton-proton collisions, at a center-of-mass energy of 13 TeV. This is a challenging task involving many detector inputs, combining fully calibrated electrons, muons, photons, hadronically decaying $\\tau$-leptons, hadronic jets, and soft activity from remaining tracks. Possible double counting of momentum is avoided by applying a signal ambiguity resolution procedure which rejects detector inputs that have already been used. Several $p_{\\text{T}}^{\\text{miss}}$ `working points' are defined "},"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":"2402.05858","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2024-02-08T17:42:34Z","cross_cats_sorted":[],"title_canon_sha256":"89568e4bb035525832ba02e13fd87b7c6a5d0607b3511974a6b2ec9397e94cf2","abstract_canon_sha256":"1f9e9d8dbb043321cc9444b70b162fac447cd6785d527e42c08c233e4ed5443a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:25:59.076755Z","signature_b64":"9pBz7hUnVPSdsFpoDK3UXTIOsrxt2veLktE/Hqnk+am1iyL6SJO8uUHBMyYvDGhCxIy+HXev5ijD6DN2wVQlAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b88f62400f58c957620bc7e76936ffb7a899e7b8394f9cb0cb8dbfc27eb0bdfc","last_reissued_at":"2026-07-05T11:25:59.076311Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:25:59.076311Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The performance of missing transverse momentum reconstruction and its significance with the ATLAS detector using 140 fb$^{-1}$ of $\\sqrt{s}=13$ TeV $pp$ collisions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2024-02-08T17:42:34Z","abstract_excerpt":"This paper presents the reconstruction of missing transverse momentum ($p_{\\text{T}}^{\\text{miss}}$) in proton-proton collisions, at a center-of-mass energy of 13 TeV. This is a challenging task involving many detector inputs, combining fully calibrated electrons, muons, photons, hadronically decaying $\\tau$-leptons, hadronic jets, and soft activity from remaining tracks. Possible double counting of momentum is avoided by applying a signal ambiguity resolution procedure which rejects detector inputs that have already been used. Several $p_{\\text{T}}^{\\text{miss}}$ `working points' are defined "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.05858","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/2402.05858/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":"2402.05858","created_at":"2026-07-05T11:25:59.076381+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.05858v2","created_at":"2026-07-05T11:25:59.076381+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.05858","created_at":"2026-07-05T11:25:59.076381+00:00"},{"alias_kind":"pith_short_12","alias_value":"XCHWEQAPLDEV","created_at":"2026-07-05T11:25:59.076381+00:00"},{"alias_kind":"pith_short_16","alias_value":"XCHWEQAPLDEVOYQL","created_at":"2026-07-05T11:25:59.076381+00:00"},{"alias_kind":"pith_short_8","alias_value":"XCHWEQAP","created_at":"2026-07-05T11:25:59.076381+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":15,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.06199","citing_title":"Simultaneous efficiency measurements of $b$- and $c$-jets in $t\\bar{t}$ events from $\\sqrt{s}=13.6$ TeV $pp$ collision data collected with the ATLAS detector","ref_index":70,"is_internal_anchor":true},{"citing_arxiv_id":"2606.04855","citing_title":"Probing the Higgs-top Yukawa interaction in the $t\\bar{t}H$ and $tH$ processes using $H\\rightarrow\\gamma\\gamma$ with the ATLAS detector","ref_index":96,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02067","citing_title":"Search for a leptoquark in events with a hadronically decaying $\\tau$-lepton and missing transverse momentum using $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":76,"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":122,"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":37,"is_internal_anchor":false},{"citing_arxiv_id":"2503.17461","citing_title":"Electroweak diboson production in association with a high-mass dijet system in semileptonic final states from $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","ref_index":95,"is_internal_anchor":false},{"citing_arxiv_id":"2504.05919","citing_title":"Measurement of high-mass $t\\bar{t}\\ell^{+}\\ell^{-}$ production and lepton flavour universality-inspired effective field theory interpretations at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":84,"is_internal_anchor":false},{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":116,"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":122,"is_internal_anchor":false},{"citing_arxiv_id":"2511.21240","citing_title":"Search for signatures of electroweakinos with photons, jets, and large missing transverse momentum in $\\sqrt{s}=13$ TeV pp collisions with the ATLAS detector","ref_index":83,"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":105,"is_internal_anchor":false},{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":116,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13819","citing_title":"Search for charginos and neutralinos with $B-L$ $R$-parity violating decays in $\\sqrt{s}=13$ TeV and $13.6$ TeV $pp$ collisions with the ATLAS detector","ref_index":97,"is_internal_anchor":false},{"citing_arxiv_id":"2605.07585","citing_title":"Track and Vertex Reconstruction with the ATLAS Inner Detector","ref_index":90,"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":55,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XCHWEQAPLDEVOYQLY7TWSNX7W6","json":"https://pith.science/pith/XCHWEQAPLDEVOYQLY7TWSNX7W6.json","graph_json":"https://pith.science/api/pith-number/XCHWEQAPLDEVOYQLY7TWSNX7W6/graph.json","events_json":"https://pith.science/api/pith-number/XCHWEQAPLDEVOYQLY7TWSNX7W6/events.json","paper":"https://pith.science/paper/XCHWEQAP"},"agent_actions":{"view_html":"https://pith.science/pith/XCHWEQAPLDEVOYQLY7TWSNX7W6","download_json":"https://pith.science/pith/XCHWEQAPLDEVOYQLY7TWSNX7W6.json","view_paper":"https://pith.science/paper/XCHWEQAP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.05858&json=true","fetch_graph":"https://pith.science/api/pith-number/XCHWEQAPLDEVOYQLY7TWSNX7W6/graph.json","fetch_events":"https://pith.science/api/pith-number/XCHWEQAPLDEVOYQLY7TWSNX7W6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XCHWEQAPLDEVOYQLY7TWSNX7W6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XCHWEQAPLDEVOYQLY7TWSNX7W6/action/storage_attestation","attest_author":"https://pith.science/pith/XCHWEQAPLDEVOYQLY7TWSNX7W6/action/author_attestation","sign_citation":"https://pith.science/pith/XCHWEQAPLDEVOYQLY7TWSNX7W6/action/citation_signature","submit_replication":"https://pith.science/pith/XCHWEQAPLDEVOYQLY7TWSNX7W6/action/replication_record"}},"created_at":"2026-07-05T11:25:59.076381+00:00","updated_at":"2026-07-05T11:25:59.076381+00:00"}