{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:A7TU6TW4GRSYBDEYA7T2OALJVW","short_pith_number":"pith:A7TU6TW4","schema_version":"1.0","canonical_sha256":"07e74f4edc3465808c9807e7a70169ad913420e65a53663799d75a591ad993ab","source":{"kind":"arxiv","id":"1909.00592","version":2},"attestation_state":"computed","paper":{"title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hamzeh Khanpour, Mojtaba Mohammadi Najafabadi, Parvin Eslami, Reza Jafari","submitted_at":"2019-09-02T08:23:09Z","abstract_excerpt":"Our main aim in this paper is to constrain the effective field theory describing the top quark couplings through the $e^{-} e^{+} \\rightarrow t \\bar{t}+$jet process. The analysis is carried out considering two different center-of-mass energies of 500 and 3000 GeV including a realistic simulation of the detector response and the main sources of background processes. The expected limits at 95\\% CL are derived on the new physics couplings such as $t \\bar t \\gamma$, $t \\bar t Z$, and $t \\bar t g$ for each benchmark scenario using the dileptonic $t \\bar{t}$ final state. We show that the 95\\% CL lim"},"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":"1909.00592","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-09-02T08:23:09Z","cross_cats_sorted":[],"title_canon_sha256":"15c5f8311f2a324342eabb48424989a78164d3e34c628b70ffe846fa4366c57e","abstract_canon_sha256":"ac94185f7f8d525683d9048286adb06b7d756d3c0db69c14654504102ef2412c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:04:46.369298Z","signature_b64":"LXe4jPeojYQ8rnBZMCgnQHxTYrPedLe8MQSAVx4UNtf5GVsry/hth3U664WIUzTgWSWJubnHePUxlcCL5maKAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07e74f4edc3465808c9807e7a70169ad913420e65a53663799d75a591ad993ab","last_reissued_at":"2026-07-05T01:04:46.368864Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:04:46.368864Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constraining the top quark effective field theory using the top quark pair production in association with a jet at future lepton colliders","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hamzeh Khanpour, Mojtaba Mohammadi Najafabadi, Parvin Eslami, Reza Jafari","submitted_at":"2019-09-02T08:23:09Z","abstract_excerpt":"Our main aim in this paper is to constrain the effective field theory describing the top quark couplings through the $e^{-} e^{+} \\rightarrow t \\bar{t}+$jet process. The analysis is carried out considering two different center-of-mass energies of 500 and 3000 GeV including a realistic simulation of the detector response and the main sources of background processes. The expected limits at 95\\% CL are derived on the new physics couplings such as $t \\bar t \\gamma$, $t \\bar t Z$, and $t \\bar t g$ for each benchmark scenario using the dileptonic $t \\bar{t}$ final state. We show that the 95\\% CL lim"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1909.00592","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1909.00592/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":"1909.00592","created_at":"2026-07-05T01:04:46.368916+00:00"},{"alias_kind":"arxiv_version","alias_value":"1909.00592v2","created_at":"2026-07-05T01:04:46.368916+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1909.00592","created_at":"2026-07-05T01:04:46.368916+00:00"},{"alias_kind":"pith_short_12","alias_value":"A7TU6TW4GRSY","created_at":"2026-07-05T01:04:46.368916+00:00"},{"alias_kind":"pith_short_16","alias_value":"A7TU6TW4GRSYBDEY","created_at":"2026-07-05T01:04:46.368916+00:00"},{"alias_kind":"pith_short_8","alias_value":"A7TU6TW4","created_at":"2026-07-05T01:04:46.368916+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/A7TU6TW4GRSYBDEYA7T2OALJVW","json":"https://pith.science/pith/A7TU6TW4GRSYBDEYA7T2OALJVW.json","graph_json":"https://pith.science/api/pith-number/A7TU6TW4GRSYBDEYA7T2OALJVW/graph.json","events_json":"https://pith.science/api/pith-number/A7TU6TW4GRSYBDEYA7T2OALJVW/events.json","paper":"https://pith.science/paper/A7TU6TW4"},"agent_actions":{"view_html":"https://pith.science/pith/A7TU6TW4GRSYBDEYA7T2OALJVW","download_json":"https://pith.science/pith/A7TU6TW4GRSYBDEYA7T2OALJVW.json","view_paper":"https://pith.science/paper/A7TU6TW4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1909.00592&json=true","fetch_graph":"https://pith.science/api/pith-number/A7TU6TW4GRSYBDEYA7T2OALJVW/graph.json","fetch_events":"https://pith.science/api/pith-number/A7TU6TW4GRSYBDEYA7T2OALJVW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A7TU6TW4GRSYBDEYA7T2OALJVW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A7TU6TW4GRSYBDEYA7T2OALJVW/action/storage_attestation","attest_author":"https://pith.science/pith/A7TU6TW4GRSYBDEYA7T2OALJVW/action/author_attestation","sign_citation":"https://pith.science/pith/A7TU6TW4GRSYBDEYA7T2OALJVW/action/citation_signature","submit_replication":"https://pith.science/pith/A7TU6TW4GRSYBDEYA7T2OALJVW/action/replication_record"}},"created_at":"2026-07-05T01:04:46.368916+00:00","updated_at":"2026-07-05T01:04:46.368916+00:00"}