{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:UIOB2NPNPRRZUEYZDPNQTKJ6OX","short_pith_number":"pith:UIOB2NPN","schema_version":"1.0","canonical_sha256":"a21c1d35ed7c639a13191bdb09a93e75feb64ea557a404dab083aec0c13478bc","source":{"kind":"arxiv","id":"1506.08845","version":2},"attestation_state":"computed","paper":{"title":"A global fit of top quark effective theory to data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andy Buckley, Chris D. White, Christoph Englert, David J. Miller, James Ferrando, Liam Moore, Michael Russell","submitted_at":"2015-06-29T20:19:24Z","abstract_excerpt":"In this paper we present a global fit of beyond the Standard Model (BSM) dimension six operators relevant to the top quark sector to currently available data. Experimental measurements include parton-level top-pair and single top production from the LHC and the Tevatron. Higher order QCD corrections are modelled using differential and global K-factors, and we use novel fast-fitting techniques developed in the context of Monte Carlo event generator tuning to perform the fit. This allows us to provide new, fully correlated and model-independent bounds on new physics effects in the top sector fro"},"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":"1506.08845","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-06-29T20:19:24Z","cross_cats_sorted":[],"title_canon_sha256":"4d31a57ef961cb679cdf311bf992ed99f165ca34711fded820faf002cd7f5a49","abstract_canon_sha256":"0773deae84c107ec0281ebef1e47ff91454ecfbf01ad46119c2733a2d2db8080"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:25:38.820870Z","signature_b64":"tXqnLKLStctDIjr+ER51zKk7lWOLX5XrwZYwzwcWn8EikvhWeJ3ciSfv/6BMJcoEOMeLqyEp0/LZM7H9R+2GDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a21c1d35ed7c639a13191bdb09a93e75feb64ea557a404dab083aec0c13478bc","last_reissued_at":"2026-05-18T01:25:38.820288Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:25:38.820288Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A global fit of top quark effective theory to data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andy Buckley, Chris D. White, Christoph Englert, David J. Miller, James Ferrando, Liam Moore, Michael Russell","submitted_at":"2015-06-29T20:19:24Z","abstract_excerpt":"In this paper we present a global fit of beyond the Standard Model (BSM) dimension six operators relevant to the top quark sector to currently available data. Experimental measurements include parton-level top-pair and single top production from the LHC and the Tevatron. Higher order QCD corrections are modelled using differential and global K-factors, and we use novel fast-fitting techniques developed in the context of Monte Carlo event generator tuning to perform the fit. This allows us to provide new, fully correlated and model-independent bounds on new physics effects in the top sector fro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.08845","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":""},"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":"1506.08845","created_at":"2026-05-18T01:25:38.820392+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.08845v2","created_at":"2026-05-18T01:25:38.820392+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.08845","created_at":"2026-05-18T01:25:38.820392+00:00"},{"alias_kind":"pith_short_12","alias_value":"UIOB2NPNPRRZ","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_16","alias_value":"UIOB2NPNPRRZUEYZ","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_8","alias_value":"UIOB2NPN","created_at":"2026-05-18T12:29:44.643036+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1906.10631","citing_title":"Towards global fits in EFT's and New Physics implications","ref_index":20,"is_internal_anchor":true},{"citing_arxiv_id":"2605.11747","citing_title":"SMEFT everywhere: a NLO study of $\\boldsymbol{pp \\to t\\bar{t}H}$ with decaying tops","ref_index":47,"is_internal_anchor":false},{"citing_arxiv_id":"2605.12033","citing_title":"Quantumness of top quark pairs produced at LHC within SMEFT framework","ref_index":71,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UIOB2NPNPRRZUEYZDPNQTKJ6OX","json":"https://pith.science/pith/UIOB2NPNPRRZUEYZDPNQTKJ6OX.json","graph_json":"https://pith.science/api/pith-number/UIOB2NPNPRRZUEYZDPNQTKJ6OX/graph.json","events_json":"https://pith.science/api/pith-number/UIOB2NPNPRRZUEYZDPNQTKJ6OX/events.json","paper":"https://pith.science/paper/UIOB2NPN"},"agent_actions":{"view_html":"https://pith.science/pith/UIOB2NPNPRRZUEYZDPNQTKJ6OX","download_json":"https://pith.science/pith/UIOB2NPNPRRZUEYZDPNQTKJ6OX.json","view_paper":"https://pith.science/paper/UIOB2NPN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.08845&json=true","fetch_graph":"https://pith.science/api/pith-number/UIOB2NPNPRRZUEYZDPNQTKJ6OX/graph.json","fetch_events":"https://pith.science/api/pith-number/UIOB2NPNPRRZUEYZDPNQTKJ6OX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UIOB2NPNPRRZUEYZDPNQTKJ6OX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UIOB2NPNPRRZUEYZDPNQTKJ6OX/action/storage_attestation","attest_author":"https://pith.science/pith/UIOB2NPNPRRZUEYZDPNQTKJ6OX/action/author_attestation","sign_citation":"https://pith.science/pith/UIOB2NPNPRRZUEYZDPNQTKJ6OX/action/citation_signature","submit_replication":"https://pith.science/pith/UIOB2NPNPRRZUEYZDPNQTKJ6OX/action/replication_record"}},"created_at":"2026-05-18T01:25:38.820392+00:00","updated_at":"2026-05-18T01:25:38.820392+00:00"}