{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:ALHXUHZ3BCFQFXKXQLUVK4KNGG","short_pith_number":"pith:ALHXUHZ3","schema_version":"1.0","canonical_sha256":"02cf7a1f3b088b02dd5782e955714d3186da4410aaf692b3460436688a6f9029","source":{"kind":"arxiv","id":"1305.7088","version":1},"attestation_state":"computed","paper":{"title":"Single-top $t$-channel production with off-shell and non-resonant effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. S. Papanastasiou, F. Maltoni, R. Frederix, S. Frixione, V. Hirschi","submitted_at":"2013-05-30T12:51:19Z","abstract_excerpt":"This letter details and discusses the next-to-leading order QCD corrections to $t$-channel electro-weak $W^+ b j$ production, where finite top-width effects are consistently taken into account. The computation is done within the aMC@NLO framework and includes both resonant and non-resonant contributions as well as interferences between the two. Results are presented for the LHC and compared to those of the narrow-width approximation and effective theory approaches."},"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":"1305.7088","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-05-30T12:51:19Z","cross_cats_sorted":[],"title_canon_sha256":"521d153b20b5d7c4a67fd18695943d1753d197baa6ffadcf00931d09f9ceb4bf","abstract_canon_sha256":"49ae5a830dfb1b300b872290ea3954ba9fb810b8ae8d3e0dd7c4729e777a25a5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:49:39.798918Z","signature_b64":"zegpWcIfng3gZ8NQC7K+U2uRjWRkXc6njlf19JhxOxsu97Ml6zYyo/x6G7IVnmYXSzYb3DQhLqgUfk5L5zCoBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"02cf7a1f3b088b02dd5782e955714d3186da4410aaf692b3460436688a6f9029","last_reissued_at":"2026-05-18T01:49:39.798373Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:49:39.798373Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Single-top $t$-channel production with off-shell and non-resonant effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. S. Papanastasiou, F. Maltoni, R. Frederix, S. Frixione, V. Hirschi","submitted_at":"2013-05-30T12:51:19Z","abstract_excerpt":"This letter details and discusses the next-to-leading order QCD corrections to $t$-channel electro-weak $W^+ b j$ production, where finite top-width effects are consistently taken into account. The computation is done within the aMC@NLO framework and includes both resonant and non-resonant contributions as well as interferences between the two. Results are presented for the LHC and compared to those of the narrow-width approximation and effective theory approaches."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.7088","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":"1305.7088","created_at":"2026-05-18T01:49:39.798457+00:00"},{"alias_kind":"arxiv_version","alias_value":"1305.7088v1","created_at":"2026-05-18T01:49:39.798457+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.7088","created_at":"2026-05-18T01:49:39.798457+00:00"},{"alias_kind":"pith_short_12","alias_value":"ALHXUHZ3BCFQ","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"ALHXUHZ3BCFQFXKX","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"ALHXUHZ3","created_at":"2026-05-18T12:27:38.830355+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"1405.0301","citing_title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","ref_index":214,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ALHXUHZ3BCFQFXKXQLUVK4KNGG","json":"https://pith.science/pith/ALHXUHZ3BCFQFXKXQLUVK4KNGG.json","graph_json":"https://pith.science/api/pith-number/ALHXUHZ3BCFQFXKXQLUVK4KNGG/graph.json","events_json":"https://pith.science/api/pith-number/ALHXUHZ3BCFQFXKXQLUVK4KNGG/events.json","paper":"https://pith.science/paper/ALHXUHZ3"},"agent_actions":{"view_html":"https://pith.science/pith/ALHXUHZ3BCFQFXKXQLUVK4KNGG","download_json":"https://pith.science/pith/ALHXUHZ3BCFQFXKXQLUVK4KNGG.json","view_paper":"https://pith.science/paper/ALHXUHZ3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1305.7088&json=true","fetch_graph":"https://pith.science/api/pith-number/ALHXUHZ3BCFQFXKXQLUVK4KNGG/graph.json","fetch_events":"https://pith.science/api/pith-number/ALHXUHZ3BCFQFXKXQLUVK4KNGG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ALHXUHZ3BCFQFXKXQLUVK4KNGG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ALHXUHZ3BCFQFXKXQLUVK4KNGG/action/storage_attestation","attest_author":"https://pith.science/pith/ALHXUHZ3BCFQFXKXQLUVK4KNGG/action/author_attestation","sign_citation":"https://pith.science/pith/ALHXUHZ3BCFQFXKXQLUVK4KNGG/action/citation_signature","submit_replication":"https://pith.science/pith/ALHXUHZ3BCFQFXKXQLUVK4KNGG/action/replication_record"}},"created_at":"2026-05-18T01:49:39.798457+00:00","updated_at":"2026-05-18T01:49:39.798457+00:00"}