{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:TG2J6OTXYINCJT232HPVOPRRKB","short_pith_number":"pith:TG2J6OTX","schema_version":"1.0","canonical_sha256":"99b49f3a77c21a24cf5bd1df573e31505a0255562b23bb3bdd76aa2c9859bf2e","source":{"kind":"arxiv","id":"1506.07369","version":3},"attestation_state":"computed","paper":{"title":"Pair Production of Scalar Leptoquarks at the LHC to NLO Parton Shower Accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Satyajit Seth, Subhadip Mitra, Tanumoy Mandal","submitted_at":"2015-06-24T14:04:36Z","abstract_excerpt":"We present the scalar leptoquark pair production process at the LHC computed at the next-to-leading order in QCD, matched to the PYTHIA parton shower using the MC@NLO formalism. We consider the leading order decay of a leptoquark to a lepton ($e,\\mu,\\tau$ or $\\nu_e,\\nu_\\mu,\\nu_\\tau$) and a jet and observe the effects of parton shower on the final states. For demonstration, we display the kinametical distributions of a selection of observables along with their scale uncertainties for the 13 TeV LHC. We also present pair production cross sections and $K$-factors using massless five-quark flavor "},"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":"1506.07369","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-06-24T14:04:36Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"e454ba279d5f575af8fe9bc29d5776fb28cf98bf86e48def86bc8f6a509cf3a8","abstract_canon_sha256":"0b9f632ebb6d09c2a2da46fd62b24e4d586fe548b566beab9e0af00684f6f3b9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:26.138608Z","signature_b64":"PqDZ5kNq2k+z1BqPGvVbtA9+2OtvBlXShnUcr+LOLu1M38/m7mjxZC5qbLdZN5S2KBrwejOsNfMIH1y5AaSNDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"99b49f3a77c21a24cf5bd1df573e31505a0255562b23bb3bdd76aa2c9859bf2e","last_reissued_at":"2026-05-18T01:20:26.137890Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:26.137890Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pair Production of Scalar Leptoquarks at the LHC to NLO Parton Shower Accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Satyajit Seth, Subhadip Mitra, Tanumoy Mandal","submitted_at":"2015-06-24T14:04:36Z","abstract_excerpt":"We present the scalar leptoquark pair production process at the LHC computed at the next-to-leading order in QCD, matched to the PYTHIA parton shower using the MC@NLO formalism. We consider the leading order decay of a leptoquark to a lepton ($e,\\mu,\\tau$ or $\\nu_e,\\nu_\\mu,\\nu_\\tau$) and a jet and observe the effects of parton shower on the final states. For demonstration, we display the kinametical distributions of a selection of observables along with their scale uncertainties for the 13 TeV LHC. We also present pair production cross sections and $K$-factors using massless five-quark flavor "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.07369","kind":"arxiv","version":3},"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":"1506.07369","created_at":"2026-05-18T01:20:26.137988+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.07369v3","created_at":"2026-05-18T01:20:26.137988+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.07369","created_at":"2026-05-18T01:20:26.137988+00:00"},{"alias_kind":"pith_short_12","alias_value":"TG2J6OTXYINC","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_16","alias_value":"TG2J6OTXYINCJT23","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_8","alias_value":"TG2J6OTX","created_at":"2026-05-18T12:29:42.218222+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.21148","citing_title":"Photon-initiated enhancements in the pair production of highly charged coloured particles","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TG2J6OTXYINCJT232HPVOPRRKB","json":"https://pith.science/pith/TG2J6OTXYINCJT232HPVOPRRKB.json","graph_json":"https://pith.science/api/pith-number/TG2J6OTXYINCJT232HPVOPRRKB/graph.json","events_json":"https://pith.science/api/pith-number/TG2J6OTXYINCJT232HPVOPRRKB/events.json","paper":"https://pith.science/paper/TG2J6OTX"},"agent_actions":{"view_html":"https://pith.science/pith/TG2J6OTXYINCJT232HPVOPRRKB","download_json":"https://pith.science/pith/TG2J6OTXYINCJT232HPVOPRRKB.json","view_paper":"https://pith.science/paper/TG2J6OTX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.07369&json=true","fetch_graph":"https://pith.science/api/pith-number/TG2J6OTXYINCJT232HPVOPRRKB/graph.json","fetch_events":"https://pith.science/api/pith-number/TG2J6OTXYINCJT232HPVOPRRKB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TG2J6OTXYINCJT232HPVOPRRKB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TG2J6OTXYINCJT232HPVOPRRKB/action/storage_attestation","attest_author":"https://pith.science/pith/TG2J6OTXYINCJT232HPVOPRRKB/action/author_attestation","sign_citation":"https://pith.science/pith/TG2J6OTXYINCJT232HPVOPRRKB/action/citation_signature","submit_replication":"https://pith.science/pith/TG2J6OTXYINCJT232HPVOPRRKB/action/replication_record"}},"created_at":"2026-05-18T01:20:26.137988+00:00","updated_at":"2026-05-18T01:20:26.137988+00:00"}