{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:XCSJGLWK25SIMZ7KAQ5WKD5X2E","short_pith_number":"pith:XCSJGLWK","schema_version":"1.0","canonical_sha256":"b8a4932ecad7648667ea043b650fb7d13bd2de8f5225347ff34a1e4e63bb5406","source":{"kind":"arxiv","id":"1303.0983","version":1},"attestation_state":"computed","paper":{"title":"Charged Higgs boson production in single top mode at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Renato Guedes, Rui Santos, Stefano Moretti","submitted_at":"2013-03-05T11:08:28Z","abstract_excerpt":"The main production mode for a light charged Higgs boson at the LHC is $pp \\to t \\bar t$, with one the top-quarks decaying to a charged Higgs and a $b$-quark. However, single top production also gives rise to final states with charged Higgs bosons. In this work we analyse how the two processes compare at the LHC@14TeV. We will be working in the framework of the two-Higgs double model, considering both a CP-conserving and a CP-violating version of the model. We conclude that the single top mode could help to constrain the parameter space in several versions of the model. We also discuss the rol"},"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":"1303.0983","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-05T11:08:28Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"c5bac9cf0bd141117c57aa943dcc6ea596530cf150e86d4d3eac57b0110faa52","abstract_canon_sha256":"99c3f2fb165d52695ee28c2e00b76785f8fe3a8675eeb7268411c7a063f34883"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:31:53.263087Z","signature_b64":"CyBGpg2erCtJfpPSZSyFiQwplS7S6zAxsMkluSQsv2Gihu7j8VhpD7itss4hB5oPqR689RPHB1OZXsSiaPdvAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b8a4932ecad7648667ea043b650fb7d13bd2de8f5225347ff34a1e4e63bb5406","last_reissued_at":"2026-05-18T03:31:53.262503Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:31:53.262503Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charged Higgs boson production in single top mode at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Renato Guedes, Rui Santos, Stefano Moretti","submitted_at":"2013-03-05T11:08:28Z","abstract_excerpt":"The main production mode for a light charged Higgs boson at the LHC is $pp \\to t \\bar t$, with one the top-quarks decaying to a charged Higgs and a $b$-quark. However, single top production also gives rise to final states with charged Higgs bosons. In this work we analyse how the two processes compare at the LHC@14TeV. We will be working in the framework of the two-Higgs double model, considering both a CP-conserving and a CP-violating version of the model. We conclude that the single top mode could help to constrain the parameter space in several versions of the model. We also discuss the rol"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.0983","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":"1303.0983","created_at":"2026-05-18T03:31:53.262593+00:00"},{"alias_kind":"arxiv_version","alias_value":"1303.0983v1","created_at":"2026-05-18T03:31:53.262593+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.0983","created_at":"2026-05-18T03:31:53.262593+00:00"},{"alias_kind":"pith_short_12","alias_value":"XCSJGLWK25SI","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_16","alias_value":"XCSJGLWK25SIMZ7K","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_8","alias_value":"XCSJGLWK","created_at":"2026-05-18T12:28:06.772260+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/XCSJGLWK25SIMZ7KAQ5WKD5X2E","json":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E.json","graph_json":"https://pith.science/api/pith-number/XCSJGLWK25SIMZ7KAQ5WKD5X2E/graph.json","events_json":"https://pith.science/api/pith-number/XCSJGLWK25SIMZ7KAQ5WKD5X2E/events.json","paper":"https://pith.science/paper/XCSJGLWK"},"agent_actions":{"view_html":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E","download_json":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E.json","view_paper":"https://pith.science/paper/XCSJGLWK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1303.0983&json=true","fetch_graph":"https://pith.science/api/pith-number/XCSJGLWK25SIMZ7KAQ5WKD5X2E/graph.json","fetch_events":"https://pith.science/api/pith-number/XCSJGLWK25SIMZ7KAQ5WKD5X2E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/action/storage_attestation","attest_author":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/action/author_attestation","sign_citation":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/action/citation_signature","submit_replication":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/action/replication_record"}},"created_at":"2026-05-18T03:31:53.262593+00:00","updated_at":"2026-05-18T03:31:53.262593+00:00"}