{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:TIW2ASVLLA4SVOKOUDWCLJSH3Q","short_pith_number":"pith:TIW2ASVL","schema_version":"1.0","canonical_sha256":"9a2da04aab58392ab94ea0ec25a647dc185527c927fbcc96a0d6ad3d5d1130fb","source":{"kind":"arxiv","id":"2308.15290","version":1},"attestation_state":"computed","paper":{"title":"A flexible and efficient approach for missing transverse momentum reconstruction","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.data-an"],"primary_cat":"hep-ex","authors_text":"Caterina Pizio, Donatella Cavalli, Douglas Schaefer, Federica Piazza, Matthew Klein, Peter Loch, Russell Smith, Sarah Williams, Silvia Resconi, Teng Jian Khoo, William Balunas","submitted_at":"2023-08-29T13:25:24Z","abstract_excerpt":"Missing transverse momentum is a crucial observable for physics at hadron colliders, being the only constraint on the kinematics of \"invisible\" objects such as neutrinos and hypothetical dark matter particles. Computing missing transverse momentum at the highest possible precision, particularly in experiments at the energy frontier, can be a challenging procedure due to ambiguities in the distribution of energy and momentum between many reconstructed particle candidates. This paper describes a novel solution for efficiently encoding information required for the computation of missing transvers"},"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":"2308.15290","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2023-08-29T13:25:24Z","cross_cats_sorted":["physics.data-an"],"title_canon_sha256":"e0cdc8fa907c03f3986c320143304a84139c8770e46714edd36582244dd70c4e","abstract_canon_sha256":"78f9a0ca04ab83fe836b8c13386605021e97174c7054692d312be3d28b14fded"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:45:46.166337Z","signature_b64":"wtLxnOwpE6FyIaRA0+NrGtp3t/rs7TNol8MkiRF5QoILo5/neVF2LZtNeYgvDxhz76ViFShwN8C4o00E7CeJBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a2da04aab58392ab94ea0ec25a647dc185527c927fbcc96a0d6ad3d5d1130fb","last_reissued_at":"2026-07-05T06:45:46.165816Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:45:46.165816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A flexible and efficient approach for missing transverse momentum reconstruction","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.data-an"],"primary_cat":"hep-ex","authors_text":"Caterina Pizio, Donatella Cavalli, Douglas Schaefer, Federica Piazza, Matthew Klein, Peter Loch, Russell Smith, Sarah Williams, Silvia Resconi, Teng Jian Khoo, William Balunas","submitted_at":"2023-08-29T13:25:24Z","abstract_excerpt":"Missing transverse momentum is a crucial observable for physics at hadron colliders, being the only constraint on the kinematics of \"invisible\" objects such as neutrinos and hypothetical dark matter particles. Computing missing transverse momentum at the highest possible precision, particularly in experiments at the energy frontier, can be a challenging procedure due to ambiguities in the distribution of energy and momentum between many reconstructed particle candidates. This paper describes a novel solution for efficiently encoding information required for the computation of missing transvers"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2308.15290","kind":"arxiv","version":1},"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/2308.15290/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":"2308.15290","created_at":"2026-07-05T06:45:46.165891+00:00"},{"alias_kind":"arxiv_version","alias_value":"2308.15290v1","created_at":"2026-07-05T06:45:46.165891+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2308.15290","created_at":"2026-07-05T06:45:46.165891+00:00"},{"alias_kind":"pith_short_12","alias_value":"TIW2ASVLLA4S","created_at":"2026-07-05T06:45:46.165891+00:00"},{"alias_kind":"pith_short_16","alias_value":"TIW2ASVLLA4SVOKO","created_at":"2026-07-05T06:45:46.165891+00:00"},{"alias_kind":"pith_short_8","alias_value":"TIW2ASVL","created_at":"2026-07-05T06:45:46.165891+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2404.06335","citing_title":"Software and computing for Run 3 of the ATLAS experiment at the LHC","ref_index":218,"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":102,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TIW2ASVLLA4SVOKOUDWCLJSH3Q","json":"https://pith.science/pith/TIW2ASVLLA4SVOKOUDWCLJSH3Q.json","graph_json":"https://pith.science/api/pith-number/TIW2ASVLLA4SVOKOUDWCLJSH3Q/graph.json","events_json":"https://pith.science/api/pith-number/TIW2ASVLLA4SVOKOUDWCLJSH3Q/events.json","paper":"https://pith.science/paper/TIW2ASVL"},"agent_actions":{"view_html":"https://pith.science/pith/TIW2ASVLLA4SVOKOUDWCLJSH3Q","download_json":"https://pith.science/pith/TIW2ASVLLA4SVOKOUDWCLJSH3Q.json","view_paper":"https://pith.science/paper/TIW2ASVL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2308.15290&json=true","fetch_graph":"https://pith.science/api/pith-number/TIW2ASVLLA4SVOKOUDWCLJSH3Q/graph.json","fetch_events":"https://pith.science/api/pith-number/TIW2ASVLLA4SVOKOUDWCLJSH3Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TIW2ASVLLA4SVOKOUDWCLJSH3Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TIW2ASVLLA4SVOKOUDWCLJSH3Q/action/storage_attestation","attest_author":"https://pith.science/pith/TIW2ASVLLA4SVOKOUDWCLJSH3Q/action/author_attestation","sign_citation":"https://pith.science/pith/TIW2ASVLLA4SVOKOUDWCLJSH3Q/action/citation_signature","submit_replication":"https://pith.science/pith/TIW2ASVLLA4SVOKOUDWCLJSH3Q/action/replication_record"}},"created_at":"2026-07-05T06:45:46.165891+00:00","updated_at":"2026-07-05T06:45:46.165891+00:00"}