{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:ICRK6WQQF3AJTDYURNXKBERUF2","short_pith_number":"pith:ICRK6WQQ","schema_version":"1.0","canonical_sha256":"40a2af5a102ec0998f148b6ea092342ea026a8b46ace60b76904aa0cdab1940d","source":{"kind":"arxiv","id":"2005.08900","version":2},"attestation_state":"computed","paper":{"title":"Search for a light charged Higgs boson in the H$^\\pm$ $\\to $ cs channel in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2020-05-18T17:18:21Z","abstract_excerpt":"A search is conducted for a low-mass charged Higgs boson produced in a top quark decay and subsequently decaying into a charm and a strange quark. The data sample was recorded in proton-proton collisions at $\\sqrt{s} =$ 13 TeV by the CMS experiment at the LHC and corresponds to an integrated luminosity of 35.9 fb$^{-1}$. The search is performed in the process of top quark pair production, where one top quark decays to a bottom quark and a charged Higgs boson, and the other to a bottom quark and a W boson. With the W boson decaying to a charged lepton (electron or muon) and a neutrino, the fina"},"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":"2005.08900","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2020-05-18T17:18:21Z","cross_cats_sorted":[],"title_canon_sha256":"3a6f4f594bbd234f9cb7af57b71e837eda436dd9ce19bd896ce999ad6a4629cd","abstract_canon_sha256":"8e6e09a7be3922d22ec3577cc63aa3a568af28cda6325a251a33eea4de4eb0ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:42:36.557759Z","signature_b64":"SIk89+Bk+L07sdFBKmZ/3r/9XRXMl0GAanL7a8ktKjUUCy8D+Xl9lHEPzfSjA/I4YQsJ1PLTfL9MnqcD0b71CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"40a2af5a102ec0998f148b6ea092342ea026a8b46ace60b76904aa0cdab1940d","last_reissued_at":"2026-07-05T01:42:36.557324Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:42:36.557324Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for a light charged Higgs boson in the H$^\\pm$ $\\to $ cs channel in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2020-05-18T17:18:21Z","abstract_excerpt":"A search is conducted for a low-mass charged Higgs boson produced in a top quark decay and subsequently decaying into a charm and a strange quark. The data sample was recorded in proton-proton collisions at $\\sqrt{s} =$ 13 TeV by the CMS experiment at the LHC and corresponds to an integrated luminosity of 35.9 fb$^{-1}$. The search is performed in the process of top quark pair production, where one top quark decays to a bottom quark and a charged Higgs boson, and the other to a bottom quark and a W boson. With the W boson decaying to a charged lepton (electron or muon) and a neutrino, the fina"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2005.08900","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2005.08900/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":"2005.08900","created_at":"2026-07-05T01:42:36.557385+00:00"},{"alias_kind":"arxiv_version","alias_value":"2005.08900v2","created_at":"2026-07-05T01:42:36.557385+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2005.08900","created_at":"2026-07-05T01:42:36.557385+00:00"},{"alias_kind":"pith_short_12","alias_value":"ICRK6WQQF3AJ","created_at":"2026-07-05T01:42:36.557385+00:00"},{"alias_kind":"pith_short_16","alias_value":"ICRK6WQQF3AJTDYU","created_at":"2026-07-05T01:42:36.557385+00:00"},{"alias_kind":"pith_short_8","alias_value":"ICRK6WQQ","created_at":"2026-07-05T01:42:36.557385+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.07094","citing_title":"Searching for a Charged Higgs Boson in Top-Quark Decays via the $WZ$ Mode","ref_index":36,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ICRK6WQQF3AJTDYURNXKBERUF2","json":"https://pith.science/pith/ICRK6WQQF3AJTDYURNXKBERUF2.json","graph_json":"https://pith.science/api/pith-number/ICRK6WQQF3AJTDYURNXKBERUF2/graph.json","events_json":"https://pith.science/api/pith-number/ICRK6WQQF3AJTDYURNXKBERUF2/events.json","paper":"https://pith.science/paper/ICRK6WQQ"},"agent_actions":{"view_html":"https://pith.science/pith/ICRK6WQQF3AJTDYURNXKBERUF2","download_json":"https://pith.science/pith/ICRK6WQQF3AJTDYURNXKBERUF2.json","view_paper":"https://pith.science/paper/ICRK6WQQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2005.08900&json=true","fetch_graph":"https://pith.science/api/pith-number/ICRK6WQQF3AJTDYURNXKBERUF2/graph.json","fetch_events":"https://pith.science/api/pith-number/ICRK6WQQF3AJTDYURNXKBERUF2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ICRK6WQQF3AJTDYURNXKBERUF2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ICRK6WQQF3AJTDYURNXKBERUF2/action/storage_attestation","attest_author":"https://pith.science/pith/ICRK6WQQF3AJTDYURNXKBERUF2/action/author_attestation","sign_citation":"https://pith.science/pith/ICRK6WQQF3AJTDYURNXKBERUF2/action/citation_signature","submit_replication":"https://pith.science/pith/ICRK6WQQF3AJTDYURNXKBERUF2/action/replication_record"}},"created_at":"2026-07-05T01:42:36.557385+00:00","updated_at":"2026-07-05T01:42:36.557385+00:00"}