{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:Z6ZAR4RN5OB3W3YMXRP3UAGQRL","short_pith_number":"pith:Z6ZAR4RN","schema_version":"1.0","canonical_sha256":"cfb208f22deb83bb6f0cbc5fba00d08af201c30e6148cec34117e7fc3d51a264","source":{"kind":"arxiv","id":"2404.15984","version":3},"attestation_state":"computed","paper":{"title":"Robust Independent Validation of Experiment and Theory: Rivet version 4 release note","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Andy Buckley, Christian Bierlich, Christian Gutschow, Jonathan Butterworth, Leif Lonnblad, Peter Richardson, Tomasz Procter, Yoran Yeh","submitted_at":"2024-04-24T17:00:24Z","abstract_excerpt":"The Rivet toolkit is the primary mechanism for phenomenological preservation of collider-physics measurements, containing both a computational core and API for analysis implementation, and a large collection of more than a thousand preserved analyses. In this note we summarise the main changes in the new Rivet 4 major release series. These include a major generalisation and more semantically coherent model for histograms and related data objects, a thorough clean-up of inelegant and legacy observable-computation tools, and new systems for extended analysis-data, incorporation of preserved mach"},"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":"2404.15984","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-24T17:00:24Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"d29173947cea6476834a92efa2560731c35ff6fc42cf39fc9eae8713d4a16c0d","abstract_canon_sha256":"6adee524a13d7c2bbbbaf63660f51cd087b0e570fb1a2dbcfec918f320149620"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:54:49.490047Z","signature_b64":"4KwaI2PPfQYs1qYqY/UcxrNzmGJ2aDgOn+AGjR20RC4PguXTNkAxsFuxp+Zf6bAvlhHtVfr4mIuINHaSTn4QDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cfb208f22deb83bb6f0cbc5fba00d08af201c30e6148cec34117e7fc3d51a264","last_reissued_at":"2026-07-05T08:54:49.489569Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:54:49.489569Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Robust Independent Validation of Experiment and Theory: Rivet version 4 release note","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Andy Buckley, Christian Bierlich, Christian Gutschow, Jonathan Butterworth, Leif Lonnblad, Peter Richardson, Tomasz Procter, Yoran Yeh","submitted_at":"2024-04-24T17:00:24Z","abstract_excerpt":"The Rivet toolkit is the primary mechanism for phenomenological preservation of collider-physics measurements, containing both a computational core and API for analysis implementation, and a large collection of more than a thousand preserved analyses. In this note we summarise the main changes in the new Rivet 4 major release series. These include a major generalisation and more semantically coherent model for histograms and related data objects, a thorough clean-up of inelegant and legacy observable-computation tools, and new systems for extended analysis-data, incorporation of preserved mach"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.15984","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/2404.15984/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":"2404.15984","created_at":"2026-07-05T08:54:49.489626+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.15984v3","created_at":"2026-07-05T08:54:49.489626+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.15984","created_at":"2026-07-05T08:54:49.489626+00:00"},{"alias_kind":"pith_short_12","alias_value":"Z6ZAR4RN5OB3","created_at":"2026-07-05T08:54:49.489626+00:00"},{"alias_kind":"pith_short_16","alias_value":"Z6ZAR4RN5OB3W3YM","created_at":"2026-07-05T08:54:49.489626+00:00"},{"alias_kind":"pith_short_8","alias_value":"Z6ZAR4RN","created_at":"2026-07-05T08:54:49.489626+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":12,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2607.06775","citing_title":"Data Preservation in High Energy Physics: Global Report 2026","ref_index":85,"is_internal_anchor":true},{"citing_arxiv_id":"2607.06059","citing_title":"A resonance-aware MC@NLO QCD+EW-matched calculation of lepton-pair production","ref_index":63,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24702","citing_title":"Reweighting Underlying Event and Colour Reconnection parameter variations in Sherpa","ref_index":42,"is_internal_anchor":false},{"citing_arxiv_id":"2606.23845","citing_title":"Polarized Deep-Inelastic Scattering with Spin Correlations in Herwig 7","ref_index":59,"is_internal_anchor":false},{"citing_arxiv_id":"2606.20798","citing_title":"Phenomenology of heavy-flavour jet angularities at hadron colliders","ref_index":91,"is_internal_anchor":false},{"citing_arxiv_id":"2606.01966","citing_title":"Reinterpreting the ATLAS HHH$\\to 6b$ Search with CheckMATE and Rivet: Validation, TRSM Benchmarks, and HL-LHC Prospects","ref_index":33,"is_internal_anchor":false},{"citing_arxiv_id":"2605.02622","citing_title":"Studying the Infrared Behaviour of Improved Logarithmic Accuracy Parton Showers with Herwig","ref_index":42,"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":118,"is_internal_anchor":false},{"citing_arxiv_id":"2507.08927","citing_title":"Deciphering compressed electroweakino excesses with MadAnalysis 5","ref_index":18,"is_internal_anchor":false},{"citing_arxiv_id":"2511.19633","citing_title":"An NLO-Matched Initial and Final State Parton Shower on a GPU","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2511.19633","citing_title":"An NLO-Matched Initial and Final State Parton Shower on a GPU","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2605.02622","citing_title":"Studying the Infrared Behaviour of Improved Logarithmic Accuracy Parton Showers with Herwig","ref_index":42,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Z6ZAR4RN5OB3W3YMXRP3UAGQRL","json":"https://pith.science/pith/Z6ZAR4RN5OB3W3YMXRP3UAGQRL.json","graph_json":"https://pith.science/api/pith-number/Z6ZAR4RN5OB3W3YMXRP3UAGQRL/graph.json","events_json":"https://pith.science/api/pith-number/Z6ZAR4RN5OB3W3YMXRP3UAGQRL/events.json","paper":"https://pith.science/paper/Z6ZAR4RN"},"agent_actions":{"view_html":"https://pith.science/pith/Z6ZAR4RN5OB3W3YMXRP3UAGQRL","download_json":"https://pith.science/pith/Z6ZAR4RN5OB3W3YMXRP3UAGQRL.json","view_paper":"https://pith.science/paper/Z6ZAR4RN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.15984&json=true","fetch_graph":"https://pith.science/api/pith-number/Z6ZAR4RN5OB3W3YMXRP3UAGQRL/graph.json","fetch_events":"https://pith.science/api/pith-number/Z6ZAR4RN5OB3W3YMXRP3UAGQRL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Z6ZAR4RN5OB3W3YMXRP3UAGQRL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Z6ZAR4RN5OB3W3YMXRP3UAGQRL/action/storage_attestation","attest_author":"https://pith.science/pith/Z6ZAR4RN5OB3W3YMXRP3UAGQRL/action/author_attestation","sign_citation":"https://pith.science/pith/Z6ZAR4RN5OB3W3YMXRP3UAGQRL/action/citation_signature","submit_replication":"https://pith.science/pith/Z6ZAR4RN5OB3W3YMXRP3UAGQRL/action/replication_record"}},"created_at":"2026-07-05T08:54:49.489626+00:00","updated_at":"2026-07-05T08:54:49.489626+00:00"}