{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:KPK6BUURTDX4W53NBYY4IV4FCU","short_pith_number":"pith:KPK6BUUR","schema_version":"1.0","canonical_sha256":"53d5e0d29198efcb776d0e31c457851529e4030bec45fd13052933db888d4464","source":{"kind":"arxiv","id":"2007.02645","version":2},"attestation_state":"computed","paper":{"title":"Jet energy scale and resolution measured 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":"2020-07-06T11:12:07Z","abstract_excerpt":"Jet energy scale and resolution measurements with their associated uncertainties are reported for jets using 36-81 fb$^{-1}$ of proton-proton collision data with a centre-of-mass energy of $\\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. Jets are reconstructed using two different input types: topo-clusters formed from energy deposits in calorimeter cells, as well as an algorithmic combination of charged-particle tracks with those topo-clusters, referred to as the ATLAS particle-flow reconstruction method. The anti-$k_t$ jet algorithm with radius parameter $R=0.4$ is the primary je"},"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":"2007.02645","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2020-07-06T11:12:07Z","cross_cats_sorted":[],"title_canon_sha256":"679dc6a0aa0c79f3e8d8505ef8c685ca61acfcdc5e0fa71c5ccdc76e6fbde0d9","abstract_canon_sha256":"2c35ef476f8a5f88fde1426656c3f68620c459c2fcdab68a6778a047d9a72c73"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:09:15.661726Z","signature_b64":"TdkNqm/2NCR5N9JqMYvvJvFHcNdz/Phk9M+maX67/LGoilupE9KCpBDuaWkCEVeWLv78tE1KGpf/dr0O7q1MAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53d5e0d29198efcb776d0e31c457851529e4030bec45fd13052933db888d4464","last_reissued_at":"2026-07-05T03:09:15.661334Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:09:15.661334Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Jet energy scale and resolution measured 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":"2020-07-06T11:12:07Z","abstract_excerpt":"Jet energy scale and resolution measurements with their associated uncertainties are reported for jets using 36-81 fb$^{-1}$ of proton-proton collision data with a centre-of-mass energy of $\\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. Jets are reconstructed using two different input types: topo-clusters formed from energy deposits in calorimeter cells, as well as an algorithmic combination of charged-particle tracks with those topo-clusters, referred to as the ATLAS particle-flow reconstruction method. The anti-$k_t$ jet algorithm with radius parameter $R=0.4$ is the primary je"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2007.02645","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/2007.02645/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":"2007.02645","created_at":"2026-07-05T03:09:15.661391+00:00"},{"alias_kind":"arxiv_version","alias_value":"2007.02645v2","created_at":"2026-07-05T03:09:15.661391+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2007.02645","created_at":"2026-07-05T03:09:15.661391+00:00"},{"alias_kind":"pith_short_12","alias_value":"KPK6BUURTDX4","created_at":"2026-07-05T03:09:15.661391+00:00"},{"alias_kind":"pith_short_16","alias_value":"KPK6BUURTDX4W53N","created_at":"2026-07-05T03:09:15.661391+00:00"},{"alias_kind":"pith_short_8","alias_value":"KPK6BUUR","created_at":"2026-07-05T03:09:15.661391+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":27,"internal_anchor_count":2,"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":67,"is_internal_anchor":true},{"citing_arxiv_id":"2607.05322","citing_title":"Measurement of the $b$-jet identification efficiency in dileptonic $t\\bar{t}$ events using proton-proton collision data at $\\sqrt{s}=13.6$ TeV collected with the ATLAS detector","ref_index":62,"is_internal_anchor":true},{"citing_arxiv_id":"2606.20463","citing_title":"Observation of centrality-dependent dijet transverse momentum imbalance in O+O and Ne+Ne collisions at $\\sqrt{s_{NN}}$ = 5.36 TeV with the ATLAS detector","ref_index":73,"is_internal_anchor":false},{"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":95,"is_internal_anchor":false},{"citing_arxiv_id":"2606.03222","citing_title":"Search for electroweak scale dijet resonances in pile-up collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":48,"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":82,"is_internal_anchor":false},{"citing_arxiv_id":"2606.31375","citing_title":"Measurement of $J/\\psi$-jet correlations in $pp$ and Pb+Pb collisions at $\\sqrt{s_{\\text{NN}}}=5.02$ TeV with the ATLAS detector","ref_index":61,"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":119,"is_internal_anchor":false},{"citing_arxiv_id":"2605.28538","citing_title":"Search for pair-produced vector-like $T$-quarks decaying into $Ht$ final states in the lepton-plus-jets channel in $pp$ collisions at $\\sqrt{s}$=13 TeV with the ATLAS detector","ref_index":89,"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":68,"is_internal_anchor":false},{"citing_arxiv_id":"2404.06335","citing_title":"Software and computing for Run 3 of the ATLAS experiment at the LHC","ref_index":31,"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":85,"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":81,"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":68,"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":107,"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":119,"is_internal_anchor":false},{"citing_arxiv_id":"2507.03495","citing_title":"Study of Higgs boson pair production in the $HH \\rightarrow b \\overline{b} \\gamma \\gamma$ final state with 308 fb$^{-1}$ of data collected at $\\sqrt{s} =$ 13 TeV and 13.6 TeV by the ATLAS experiment","ref_index":99,"is_internal_anchor":false},{"citing_arxiv_id":"2509.13759","citing_title":"Measurement of the $W$-boson angular coefficients and transverse momentum in $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector","ref_index":81,"is_internal_anchor":false},{"citing_arxiv_id":"2509.14005","citing_title":"Search for Higgs bosons produced in association with a high-energy photon via vector-boson fusion and decaying to a pair of $b$-quarks in the ATLAS detector","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2509.14070","citing_title":"Observation of $W^{+}W^{-}\\gamma$ production in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector and constraints on anomalous quartic gauge-boson couplings","ref_index":69,"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":103,"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":107,"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":93,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24435","citing_title":"Measurement of jet photoproduction in ultra-peripheral Pb+Pb collisions without nuclear breakup at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV with the ATLAS detector","ref_index":58,"is_internal_anchor":false},{"citing_arxiv_id":"2605.07585","citing_title":"Track and Vertex Reconstruction with the ATLAS Inner Detector","ref_index":109,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KPK6BUURTDX4W53NBYY4IV4FCU","json":"https://pith.science/pith/KPK6BUURTDX4W53NBYY4IV4FCU.json","graph_json":"https://pith.science/api/pith-number/KPK6BUURTDX4W53NBYY4IV4FCU/graph.json","events_json":"https://pith.science/api/pith-number/KPK6BUURTDX4W53NBYY4IV4FCU/events.json","paper":"https://pith.science/paper/KPK6BUUR"},"agent_actions":{"view_html":"https://pith.science/pith/KPK6BUURTDX4W53NBYY4IV4FCU","download_json":"https://pith.science/pith/KPK6BUURTDX4W53NBYY4IV4FCU.json","view_paper":"https://pith.science/paper/KPK6BUUR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2007.02645&json=true","fetch_graph":"https://pith.science/api/pith-number/KPK6BUURTDX4W53NBYY4IV4FCU/graph.json","fetch_events":"https://pith.science/api/pith-number/KPK6BUURTDX4W53NBYY4IV4FCU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KPK6BUURTDX4W53NBYY4IV4FCU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KPK6BUURTDX4W53NBYY4IV4FCU/action/storage_attestation","attest_author":"https://pith.science/pith/KPK6BUURTDX4W53NBYY4IV4FCU/action/author_attestation","sign_citation":"https://pith.science/pith/KPK6BUURTDX4W53NBYY4IV4FCU/action/citation_signature","submit_replication":"https://pith.science/pith/KPK6BUURTDX4W53NBYY4IV4FCU/action/replication_record"}},"created_at":"2026-07-05T03:09:15.661391+00:00","updated_at":"2026-07-05T03:09:15.661391+00:00"}