{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:24K5ZBBUQYJRCUKA7ZZE3JDM2F","short_pith_number":"pith:24K5ZBBU","schema_version":"1.0","canonical_sha256":"d715dc84348613115140fe724da46cd142873d601021d20d6b779a61f38f2778","source":{"kind":"arxiv","id":"1907.04343","version":1},"attestation_state":"computed","paper":{"title":"Top-quark pair hadroproduction in association with a heavy boson at NLO+NNLL including EW corrections","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alessandro Broggio, Andrea Ferroglia, Benjamin D. Pecjak, Davide Pagani, Ioannis Tsinikos, Rikkert Frederix","submitted_at":"2019-07-09T18:03:08Z","abstract_excerpt":"This work studies the associated production of a top-quark pair with a $W$, $Z$, or Higgs boson at the LHC. Predictions for the total cross sections as well as for several differential distributions of the massive particles in the final state are provided. These predictions, valid for the LHC operating at $13$ TeV, include without any approximation all the NLO electroweak and QCD contributions of $\\mathcal{O}(\\alpha_s^{i} \\alpha^{j+1})$ with $i+j=2,3$. In addition, the predictions presented here improve upon the NLO QCD results by adding the effects of soft gluon emission corrections resummed "},"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":"1907.04343","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-07-09T18:03:08Z","cross_cats_sorted":[],"title_canon_sha256":"f5187a0c969e4ac6ea06411e29db41d90c35f17bdb487dabb10f271dad12a2a5","abstract_canon_sha256":"2bbb7576edb95497e2b3fbd22dd45126314acd7505f69e49870d7111b2e1150f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:01:58.930351Z","signature_b64":"F9JI4/4nS++Wn9MPdvfj6eNvzqoay0k/Hy9iC8vE9ZYZuL+QLZ8IF1dC0Pl0HvvZNblboOc+6E47vq6rdj8sBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d715dc84348613115140fe724da46cd142873d601021d20d6b779a61f38f2778","last_reissued_at":"2026-07-05T00:01:58.929896Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:01:58.929896Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Top-quark pair hadroproduction in association with a heavy boson at NLO+NNLL including EW corrections","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alessandro Broggio, Andrea Ferroglia, Benjamin D. Pecjak, Davide Pagani, Ioannis Tsinikos, Rikkert Frederix","submitted_at":"2019-07-09T18:03:08Z","abstract_excerpt":"This work studies the associated production of a top-quark pair with a $W$, $Z$, or Higgs boson at the LHC. Predictions for the total cross sections as well as for several differential distributions of the massive particles in the final state are provided. These predictions, valid for the LHC operating at $13$ TeV, include without any approximation all the NLO electroweak and QCD contributions of $\\mathcal{O}(\\alpha_s^{i} \\alpha^{j+1})$ with $i+j=2,3$. In addition, the predictions presented here improve upon the NLO QCD results by adding the effects of soft gluon emission corrections resummed "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1907.04343","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1907.04343/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":"1907.04343","created_at":"2026-07-05T00:01:58.929956+00:00"},{"alias_kind":"arxiv_version","alias_value":"1907.04343v1","created_at":"2026-07-05T00:01:58.929956+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1907.04343","created_at":"2026-07-05T00:01:58.929956+00:00"},{"alias_kind":"pith_short_12","alias_value":"24K5ZBBUQYJR","created_at":"2026-07-05T00:01:58.929956+00:00"},{"alias_kind":"pith_short_16","alias_value":"24K5ZBBUQYJRCUKA","created_at":"2026-07-05T00:01:58.929956+00:00"},{"alias_kind":"pith_short_8","alias_value":"24K5ZBBU","created_at":"2026-07-05T00:01:58.929956+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.09503","citing_title":"NNLO QCD predictions for $t\\bar t W$ production at hadron colliders","ref_index":9,"is_internal_anchor":false},{"citing_arxiv_id":"2606.31823","citing_title":"NNLO QCD predictions for $t\\bar{t}W$ production at the LHC","ref_index":9,"is_internal_anchor":false},{"citing_arxiv_id":"2605.05880","citing_title":"Top-associated Higgs-boson production using perturbative fragmentation functions at next-to-leading-order","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2605.05880","citing_title":"Top-associated Higgs-boson production using perturbative fragmentation functions at next-to-leading-order","ref_index":21,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/24K5ZBBUQYJRCUKA7ZZE3JDM2F","json":"https://pith.science/pith/24K5ZBBUQYJRCUKA7ZZE3JDM2F.json","graph_json":"https://pith.science/api/pith-number/24K5ZBBUQYJRCUKA7ZZE3JDM2F/graph.json","events_json":"https://pith.science/api/pith-number/24K5ZBBUQYJRCUKA7ZZE3JDM2F/events.json","paper":"https://pith.science/paper/24K5ZBBU"},"agent_actions":{"view_html":"https://pith.science/pith/24K5ZBBUQYJRCUKA7ZZE3JDM2F","download_json":"https://pith.science/pith/24K5ZBBUQYJRCUKA7ZZE3JDM2F.json","view_paper":"https://pith.science/paper/24K5ZBBU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1907.04343&json=true","fetch_graph":"https://pith.science/api/pith-number/24K5ZBBUQYJRCUKA7ZZE3JDM2F/graph.json","fetch_events":"https://pith.science/api/pith-number/24K5ZBBUQYJRCUKA7ZZE3JDM2F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/24K5ZBBUQYJRCUKA7ZZE3JDM2F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/24K5ZBBUQYJRCUKA7ZZE3JDM2F/action/storage_attestation","attest_author":"https://pith.science/pith/24K5ZBBUQYJRCUKA7ZZE3JDM2F/action/author_attestation","sign_citation":"https://pith.science/pith/24K5ZBBUQYJRCUKA7ZZE3JDM2F/action/citation_signature","submit_replication":"https://pith.science/pith/24K5ZBBUQYJRCUKA7ZZE3JDM2F/action/replication_record"}},"created_at":"2026-07-05T00:01:58.929956+00:00","updated_at":"2026-07-05T00:01:58.929956+00:00"}