{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:XH2RNQOPN33NLGPEUUZJ4UHJYK","short_pith_number":"pith:XH2RNQOP","schema_version":"1.0","canonical_sha256":"b9f516c1cf6ef6d599e4a5329e50e9c2885761d2d455c997e7293e3c4bc7b045","source":{"kind":"arxiv","id":"2404.06335","version":3},"attestation_state":"computed","paper":{"title":"Software and computing for Run 3 of the ATLAS experiment at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2024-04-09T14:19:45Z","abstract_excerpt":"The ATLAS experiment has developed extensive software and distributed computing systems for Run 3 of the LHC. These systems are described in detail, including software infrastructure and workflows, distributed data and workload management, database infrastructure, and validation. The use of these systems to prepare the data for physics analysis and assess its quality are described, along with the software tools used for data analysis itself. An outlook for the development of these projects towards Run 4 is also provided."},"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":"2404.06335","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2024-04-09T14:19:45Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"d03aac5f735b842b848defbe249afa05f4ca3ce217f3c285b3fd04bc965f7ea0","abstract_canon_sha256":"5fdc48659466987b8d508e999511a7c2e0e697f6cc801fd18490e5d19fd59297"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-22T22:48:19.925421Z","signature_b64":"TiWnqN5E3bk4UmC5S04pqXHjuspBq5WUD73wyy0AkCC+thSohGD2qwSaMdE7DNS0E9JolAedw22V81ShnxvHAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b9f516c1cf6ef6d599e4a5329e50e9c2885761d2d455c997e7293e3c4bc7b045","last_reissued_at":"2026-05-22T22:48:19.922703Z","signature_status":"signed_v1","first_computed_at":"2026-05-22T22:48:19.922703Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Software and computing for Run 3 of the ATLAS experiment at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2024-04-09T14:19:45Z","abstract_excerpt":"The ATLAS experiment has developed extensive software and distributed computing systems for Run 3 of the LHC. These systems are described in detail, including software infrastructure and workflows, distributed data and workload management, database infrastructure, and validation. The use of these systems to prepare the data for physics analysis and assess its quality are described, along with the software tools used for data analysis itself. An outlook for the development of these projects towards Run 4 is also provided."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.06335","kind":"arxiv","version":3},"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/2404.06335/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":"2404.06335","created_at":"2026-05-22T22:48:19.922812+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.06335v3","created_at":"2026-05-22T22:48:19.922812+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.06335","created_at":"2026-05-22T22:48:19.922812+00:00"},{"alias_kind":"pith_short_12","alias_value":"XH2RNQOPN33N","created_at":"2026-05-22T22:48:19.922812+00:00"},{"alias_kind":"pith_short_16","alias_value":"XH2RNQOPN33NLGPE","created_at":"2026-05-22T22:48:19.922812+00:00"},{"alias_kind":"pith_short_8","alias_value":"XH2RNQOP","created_at":"2026-05-22T22:48:19.922812+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":25,"internal_anchor_count":25,"sample":[{"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":24,"is_internal_anchor":true},{"citing_arxiv_id":"2503.05463","citing_title":"Search for Higgs boson exotic decays into Lorentz-boosted light bosons in the four-$\\tau$ final state at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":39,"is_internal_anchor":true},{"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":35,"is_internal_anchor":true},{"citing_arxiv_id":"2504.02638","citing_title":"Characterization of nuclear breakup as a function of hard-scattering kinematics using dijets measured by ATLAS in $p$+Pb collisions","ref_index":36,"is_internal_anchor":true},{"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":36,"is_internal_anchor":true},{"citing_arxiv_id":"2505.08530","citing_title":"The environmental impact, carbon emissions and sustainability of computing in the ATLAS experiment","ref_index":7,"is_internal_anchor":true},{"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":24,"is_internal_anchor":true},{"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":41,"is_internal_anchor":true},{"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":30,"is_internal_anchor":true},{"citing_arxiv_id":"2605.20015","citing_title":"Search for soft unclustered energy patterns containing muons in the final state in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16228","citing_title":"Observation of a $B_c^{*+}$ meson with the ATLAS detector","ref_index":39,"is_internal_anchor":true},{"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":53,"is_internal_anchor":true},{"citing_arxiv_id":"2509.04135","citing_title":"Measurement of coherent exclusive $J/\\psi\\to\\mu^+\\mu^-$ production in ultraperipheral Pb+Pb collisions at $\\sqrt{s_{\\textrm{NN}}}=5.36$ TeV with the ATLAS detector","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2509.05171","citing_title":"Measurement of the azimuthal anisotropy of charged particles in $\\sqrt{s_{\\mathrm{NN}}}=5.36$ TeV $^{16}$O$+^{16}$O and $^{20}$Ne$+^{20}$Ne collisions with the ATLAS detector","ref_index":50,"is_internal_anchor":true},{"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":29,"is_internal_anchor":true},{"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":10,"is_internal_anchor":true},{"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":40,"is_internal_anchor":true},{"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":29,"is_internal_anchor":true},{"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":41,"is_internal_anchor":true},{"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":27,"is_internal_anchor":true},{"citing_arxiv_id":"2605.05030","citing_title":"Study of Particle Fluence Effects on Collected Charge and Depletion Voltage of the ATLAS IBL Planar Pixel Sensors","ref_index":22,"is_internal_anchor":true},{"citing_arxiv_id":"2605.07585","citing_title":"Track and Vertex Reconstruction with the ATLAS Inner Detector","ref_index":35,"is_internal_anchor":true},{"citing_arxiv_id":"2604.05512","citing_title":"Measurement of charged-particle production in $\\sqrt{s_\\text{NN}}=9.62$ TeV proton-oxygen collisions as a probe of cosmic-ray air showers with the ATLAS detector","ref_index":121,"is_internal_anchor":true},{"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":32,"is_internal_anchor":true},{"citing_arxiv_id":"2604.20559","citing_title":"Observation of impact parameter dependent modifications of nuclear parton distributions in photonuclear Pb+Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV with the ATLAS detector","ref_index":38,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XH2RNQOPN33NLGPEUUZJ4UHJYK","json":"https://pith.science/pith/XH2RNQOPN33NLGPEUUZJ4UHJYK.json","graph_json":"https://pith.science/api/pith-number/XH2RNQOPN33NLGPEUUZJ4UHJYK/graph.json","events_json":"https://pith.science/api/pith-number/XH2RNQOPN33NLGPEUUZJ4UHJYK/events.json","paper":"https://pith.science/paper/XH2RNQOP"},"agent_actions":{"view_html":"https://pith.science/pith/XH2RNQOPN33NLGPEUUZJ4UHJYK","download_json":"https://pith.science/pith/XH2RNQOPN33NLGPEUUZJ4UHJYK.json","view_paper":"https://pith.science/paper/XH2RNQOP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.06335&json=true","fetch_graph":"https://pith.science/api/pith-number/XH2RNQOPN33NLGPEUUZJ4UHJYK/graph.json","fetch_events":"https://pith.science/api/pith-number/XH2RNQOPN33NLGPEUUZJ4UHJYK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XH2RNQOPN33NLGPEUUZJ4UHJYK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XH2RNQOPN33NLGPEUUZJ4UHJYK/action/storage_attestation","attest_author":"https://pith.science/pith/XH2RNQOPN33NLGPEUUZJ4UHJYK/action/author_attestation","sign_citation":"https://pith.science/pith/XH2RNQOPN33NLGPEUUZJ4UHJYK/action/citation_signature","submit_replication":"https://pith.science/pith/XH2RNQOPN33NLGPEUUZJ4UHJYK/action/replication_record"}},"created_at":"2026-05-22T22:48:19.922812+00:00","updated_at":"2026-05-22T22:48:19.922812+00:00"}