{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:WX5CCTS2ZO5UWIPRGGNXUK2LY5","short_pith_number":"pith:WX5CCTS2","schema_version":"1.0","canonical_sha256":"b5fa214e5acbbb4b21f1319b7a2b4bc77c72e7abf097fc243bea83e9a2de839f","source":{"kind":"arxiv","id":"1704.05478","version":2},"attestation_state":"computed","paper":{"title":"Constraints on top quark non-standard interactions from Higgs and $t \\bar t$ production cross sections","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Tonero, D. Barducci, M. Fabbrichesi","submitted_at":"2017-04-18T18:04:42Z","abstract_excerpt":"We identify the differential cross sections for $t\\bar t$ production and the total cross section for Higgs production through gluon fusion as the processes in which the two effective operators describing the leading non-standard interactions of the top quark with the gluon can be disentangled and studied in an independent fashion. Current data on the Higgs production and the $ {\\rm d}\\sigma/{\\rm d} {p^t_T}$ differential cross section provide limits comparable, but not more stringent, than those from the total $t\\bar t$ cross sections measurements at the LHC and Tevatron, where however the two "},"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":"1704.05478","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-18T18:04:42Z","cross_cats_sorted":[],"title_canon_sha256":"dae77d3a6bbbb214076862e6f4f7a6d70b046362fac1e7b1bfeebb9e8a178ec9","abstract_canon_sha256":"638d3921db4d99221bed30ffd0a26e891d1ef7afe98764b2a4b8206b3384347c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:10.736690Z","signature_b64":"14oHm1d4d6DWyu5Q14/KhwgjZ++FQOoteP2A7HLM7NGn2SdhTQEMes7D/kB0uXTGz+OWTYEQ5LV4+dTuxQuhAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b5fa214e5acbbb4b21f1319b7a2b4bc77c72e7abf097fc243bea83e9a2de839f","last_reissued_at":"2026-05-18T00:32:10.735963Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:10.735963Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constraints on top quark non-standard interactions from Higgs and $t \\bar t$ production cross sections","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Tonero, D. Barducci, M. Fabbrichesi","submitted_at":"2017-04-18T18:04:42Z","abstract_excerpt":"We identify the differential cross sections for $t\\bar t$ production and the total cross section for Higgs production through gluon fusion as the processes in which the two effective operators describing the leading non-standard interactions of the top quark with the gluon can be disentangled and studied in an independent fashion. Current data on the Higgs production and the $ {\\rm d}\\sigma/{\\rm d} {p^t_T}$ differential cross section provide limits comparable, but not more stringent, than those from the total $t\\bar t$ cross sections measurements at the LHC and Tevatron, where however the two "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.05478","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":"1704.05478","created_at":"2026-05-18T00:32:10.736085+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.05478v2","created_at":"2026-05-18T00:32:10.736085+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.05478","created_at":"2026-05-18T00:32:10.736085+00:00"},{"alias_kind":"pith_short_12","alias_value":"WX5CCTS2ZO5U","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_16","alias_value":"WX5CCTS2ZO5UWIPR","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_8","alias_value":"WX5CCTS2","created_at":"2026-05-18T12:31:53.515858+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.06996","citing_title":"Top-quark Partial Compositeness beyond the effective field theory paradigm","ref_index":35,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WX5CCTS2ZO5UWIPRGGNXUK2LY5","json":"https://pith.science/pith/WX5CCTS2ZO5UWIPRGGNXUK2LY5.json","graph_json":"https://pith.science/api/pith-number/WX5CCTS2ZO5UWIPRGGNXUK2LY5/graph.json","events_json":"https://pith.science/api/pith-number/WX5CCTS2ZO5UWIPRGGNXUK2LY5/events.json","paper":"https://pith.science/paper/WX5CCTS2"},"agent_actions":{"view_html":"https://pith.science/pith/WX5CCTS2ZO5UWIPRGGNXUK2LY5","download_json":"https://pith.science/pith/WX5CCTS2ZO5UWIPRGGNXUK2LY5.json","view_paper":"https://pith.science/paper/WX5CCTS2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.05478&json=true","fetch_graph":"https://pith.science/api/pith-number/WX5CCTS2ZO5UWIPRGGNXUK2LY5/graph.json","fetch_events":"https://pith.science/api/pith-number/WX5CCTS2ZO5UWIPRGGNXUK2LY5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WX5CCTS2ZO5UWIPRGGNXUK2LY5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WX5CCTS2ZO5UWIPRGGNXUK2LY5/action/storage_attestation","attest_author":"https://pith.science/pith/WX5CCTS2ZO5UWIPRGGNXUK2LY5/action/author_attestation","sign_citation":"https://pith.science/pith/WX5CCTS2ZO5UWIPRGGNXUK2LY5/action/citation_signature","submit_replication":"https://pith.science/pith/WX5CCTS2ZO5UWIPRGGNXUK2LY5/action/replication_record"}},"created_at":"2026-05-18T00:32:10.736085+00:00","updated_at":"2026-05-18T00:32:10.736085+00:00"}