{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:A37ISXFRHUMPX46577IYVUK32B","short_pith_number":"pith:A37ISXFR","schema_version":"1.0","canonical_sha256":"06fe895cb13d18fbf3ddffd18ad15bd07c28b42524a1c96c95968501f1b6a990","source":{"kind":"arxiv","id":"1207.5069","version":1},"attestation_state":"computed","paper":{"title":"New physics signal in top physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Celine Degrande","submitted_at":"2012-07-20T22:10:15Z","abstract_excerpt":"Effective field theories provide a model independent parametrization of the physics beyond the SM if the new degrees of freedom are heavy and complement thus the searches for resonances. In this talk, I will apply this method to the top sector which is expected to play a special role in many BSM scenarios. I will then show the effects of those dimension-six operators on cross-sections and distributions at hadron colliders. Those results together with the present data from the LHC and the Tevatron already constrain the parameter space"},"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":"1207.5069","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-07-20T22:10:15Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"88aa4bba4870f7c1057d334a4580e004600e91ac5c62fc6a59e4bd7ee298372f","abstract_canon_sha256":"4a0ab1c86b971bbcfcbfd31148b516e93dfd20aad6abb3e4dd67ca4e546bfc4a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:50:24.692795Z","signature_b64":"LcB6sZPcb9BrglQcMkGji59JZLU9MRuhx6DFtBzFAJSSoJGwMv6Gq/wmke+nOW3XtHS6qO2lmHJnthoYJPelCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"06fe895cb13d18fbf3ddffd18ad15bd07c28b42524a1c96c95968501f1b6a990","last_reissued_at":"2026-05-18T03:50:24.692024Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:50:24.692024Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New physics signal in top physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Celine Degrande","submitted_at":"2012-07-20T22:10:15Z","abstract_excerpt":"Effective field theories provide a model independent parametrization of the physics beyond the SM if the new degrees of freedom are heavy and complement thus the searches for resonances. In this talk, I will apply this method to the top sector which is expected to play a special role in many BSM scenarios. I will then show the effects of those dimension-six operators on cross-sections and distributions at hadron colliders. Those results together with the present data from the LHC and the Tevatron already constrain the parameter space"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.5069","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":""},"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":"1207.5069","created_at":"2026-05-18T03:50:24.692149+00:00"},{"alias_kind":"arxiv_version","alias_value":"1207.5069v1","created_at":"2026-05-18T03:50:24.692149+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.5069","created_at":"2026-05-18T03:50:24.692149+00:00"},{"alias_kind":"pith_short_12","alias_value":"A37ISXFRHUMP","created_at":"2026-05-18T12:26:58.693483+00:00"},{"alias_kind":"pith_short_16","alias_value":"A37ISXFRHUMPX465","created_at":"2026-05-18T12:26:58.693483+00:00"},{"alias_kind":"pith_short_8","alias_value":"A37ISXFR","created_at":"2026-05-18T12:26:58.693483+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/A37ISXFRHUMPX46577IYVUK32B","json":"https://pith.science/pith/A37ISXFRHUMPX46577IYVUK32B.json","graph_json":"https://pith.science/api/pith-number/A37ISXFRHUMPX46577IYVUK32B/graph.json","events_json":"https://pith.science/api/pith-number/A37ISXFRHUMPX46577IYVUK32B/events.json","paper":"https://pith.science/paper/A37ISXFR"},"agent_actions":{"view_html":"https://pith.science/pith/A37ISXFRHUMPX46577IYVUK32B","download_json":"https://pith.science/pith/A37ISXFRHUMPX46577IYVUK32B.json","view_paper":"https://pith.science/paper/A37ISXFR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1207.5069&json=true","fetch_graph":"https://pith.science/api/pith-number/A37ISXFRHUMPX46577IYVUK32B/graph.json","fetch_events":"https://pith.science/api/pith-number/A37ISXFRHUMPX46577IYVUK32B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A37ISXFRHUMPX46577IYVUK32B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A37ISXFRHUMPX46577IYVUK32B/action/storage_attestation","attest_author":"https://pith.science/pith/A37ISXFRHUMPX46577IYVUK32B/action/author_attestation","sign_citation":"https://pith.science/pith/A37ISXFRHUMPX46577IYVUK32B/action/citation_signature","submit_replication":"https://pith.science/pith/A37ISXFRHUMPX46577IYVUK32B/action/replication_record"}},"created_at":"2026-05-18T03:50:24.692149+00:00","updated_at":"2026-05-18T03:50:24.692149+00:00"}