{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:T7L7MQ6AQRVFS6XRNGGHGBXQJ6","short_pith_number":"pith:T7L7MQ6A","schema_version":"1.0","canonical_sha256":"9fd7f643c0846a597af1698c7306f04fa90ae7c0aaca83d89623e1e5cca1c362","source":{"kind":"arxiv","id":"1903.01646","version":2},"attestation_state":"computed","paper":{"title":"Momentum-space threshold resummation in $tW$ production at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chong Sheng Li, Ding Yu Shao, Hai Tao Li, Jian Wang","submitted_at":"2019-03-05T03:32:19Z","abstract_excerpt":"We calculate the soft-gluon corrections for $tW$ production to all orders. The soft limit is defined in the pair invariant mass or one particle inclusive kinematic schemes. We find that at NLO the contribution of the soft-gluon effect dominates in the total cross section or the differential distributions. After resumming the soft-gluon effect to all orders using the renormalization group equation, we find that the NLO+NNLL results increase the NLO cross sections by $12\\%\\sim 17\\%$ depending on the scheme and the collider energy. Our results are in agreement with the measurements at the 8 and 1"},"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":"1903.01646","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-03-05T03:32:19Z","cross_cats_sorted":[],"title_canon_sha256":"4b98eb948e6c8afe885d82c42c420a23d2eacdcc4497fcb76f5469e45ef142bc","abstract_canon_sha256":"43534b7c6b2119857933b8361c7725a35d039f4eeff8278673ecb4590098e4b9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:42:23.108556Z","signature_b64":"4m41Of/Gf0sizfYrM3usCdxu38VMcdxkzD0Qn8s8qjrr92aCF2vBLqs8R+BTzOQcdfqd3G28rF5v3jypkBQhBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9fd7f643c0846a597af1698c7306f04fa90ae7c0aaca83d89623e1e5cca1c362","last_reissued_at":"2026-05-17T23:42:23.107881Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:42:23.107881Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Momentum-space threshold resummation in $tW$ production at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chong Sheng Li, Ding Yu Shao, Hai Tao Li, Jian Wang","submitted_at":"2019-03-05T03:32:19Z","abstract_excerpt":"We calculate the soft-gluon corrections for $tW$ production to all orders. The soft limit is defined in the pair invariant mass or one particle inclusive kinematic schemes. We find that at NLO the contribution of the soft-gluon effect dominates in the total cross section or the differential distributions. After resumming the soft-gluon effect to all orders using the renormalization group equation, we find that the NLO+NNLL results increase the NLO cross sections by $12\\%\\sim 17\\%$ depending on the scheme and the collider energy. Our results are in agreement with the measurements at the 8 and 1"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1903.01646","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":"1903.01646","created_at":"2026-05-17T23:42:23.107989+00:00"},{"alias_kind":"arxiv_version","alias_value":"1903.01646v2","created_at":"2026-05-17T23:42:23.107989+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1903.01646","created_at":"2026-05-17T23:42:23.107989+00:00"},{"alias_kind":"pith_short_12","alias_value":"T7L7MQ6AQRVF","created_at":"2026-05-18T12:33:27.125529+00:00"},{"alias_kind":"pith_short_16","alias_value":"T7L7MQ6AQRVFS6XR","created_at":"2026-05-18T12:33:27.125529+00:00"},{"alias_kind":"pith_short_8","alias_value":"T7L7MQ6A","created_at":"2026-05-18T12:33:27.125529+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.21040","citing_title":"Constraining dimension-6 SMEFT with higher-order predictions for $p p \\to t W$","ref_index":106,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/T7L7MQ6AQRVFS6XRNGGHGBXQJ6","json":"https://pith.science/pith/T7L7MQ6AQRVFS6XRNGGHGBXQJ6.json","graph_json":"https://pith.science/api/pith-number/T7L7MQ6AQRVFS6XRNGGHGBXQJ6/graph.json","events_json":"https://pith.science/api/pith-number/T7L7MQ6AQRVFS6XRNGGHGBXQJ6/events.json","paper":"https://pith.science/paper/T7L7MQ6A"},"agent_actions":{"view_html":"https://pith.science/pith/T7L7MQ6AQRVFS6XRNGGHGBXQJ6","download_json":"https://pith.science/pith/T7L7MQ6AQRVFS6XRNGGHGBXQJ6.json","view_paper":"https://pith.science/paper/T7L7MQ6A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1903.01646&json=true","fetch_graph":"https://pith.science/api/pith-number/T7L7MQ6AQRVFS6XRNGGHGBXQJ6/graph.json","fetch_events":"https://pith.science/api/pith-number/T7L7MQ6AQRVFS6XRNGGHGBXQJ6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T7L7MQ6AQRVFS6XRNGGHGBXQJ6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T7L7MQ6AQRVFS6XRNGGHGBXQJ6/action/storage_attestation","attest_author":"https://pith.science/pith/T7L7MQ6AQRVFS6XRNGGHGBXQJ6/action/author_attestation","sign_citation":"https://pith.science/pith/T7L7MQ6AQRVFS6XRNGGHGBXQJ6/action/citation_signature","submit_replication":"https://pith.science/pith/T7L7MQ6AQRVFS6XRNGGHGBXQJ6/action/replication_record"}},"created_at":"2026-05-17T23:42:23.107989+00:00","updated_at":"2026-05-17T23:42:23.107989+00:00"}