{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:NFNIWPBH43UDJ6YHJUFMWK73AS","short_pith_number":"pith:NFNIWPBH","schema_version":"1.0","canonical_sha256":"695a8b3c27e6e834fb074d0acb2bfb0484d41772ff3d5970f76529197bd61c58","source":{"kind":"arxiv","id":"2008.09835","version":2},"attestation_state":"computed","paper":{"title":"A search for bottom-type, vector-like quark pair production in a fully hadronic final state 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":"2020-08-22T13:37:12Z","abstract_excerpt":"A search is described for the production of a pair of bottom-type vector-like quarks (VLQs), each decaying into a b or $\\mathrm{\\bar{b}}$ quark and either a Higgs or a Z boson, with a mass greater than 1000 GeV. The analysis is based on data from proton-proton collisions at a 13 TeV center-of-mass energy recorded at the CERN LHC, corresponding to a total integrated luminosity of 137 fb$^{-1}$. As the predominant decay modes of the Higgs and Z bosons are to a pair of quarks, the analysis focuses on final states consisting of jets resulting from the six quarks produced in the events. Since the t"},"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":"2008.09835","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2020-08-22T13:37:12Z","cross_cats_sorted":[],"title_canon_sha256":"d324c5353e9eb09d68131e8bc7acdd22cfb834c05d3b78a1f5f316535c329195","abstract_canon_sha256":"36e8d081083e98c3ea8cb62d2335a9c6d816268d2c8919a91552d289628429a8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:03:41.199335Z","signature_b64":"Fk2YPSUrHD73m+ANY6krbBL3mqKIZ0xzfbHcqBHhy1iwZN7Bk7d7L2KwUK+X79zTnzX6Pj6oEU5ysisu5pGwAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"695a8b3c27e6e834fb074d0acb2bfb0484d41772ff3d5970f76529197bd61c58","last_reissued_at":"2026-07-05T02:03:41.198889Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:03:41.198889Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A search for bottom-type, vector-like quark pair production in a fully hadronic final state 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":"2020-08-22T13:37:12Z","abstract_excerpt":"A search is described for the production of a pair of bottom-type vector-like quarks (VLQs), each decaying into a b or $\\mathrm{\\bar{b}}$ quark and either a Higgs or a Z boson, with a mass greater than 1000 GeV. The analysis is based on data from proton-proton collisions at a 13 TeV center-of-mass energy recorded at the CERN LHC, corresponding to a total integrated luminosity of 137 fb$^{-1}$. As the predominant decay modes of the Higgs and Z bosons are to a pair of quarks, the analysis focuses on final states consisting of jets resulting from the six quarks produced in the events. Since the t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2008.09835","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/2008.09835/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":"2008.09835","created_at":"2026-07-05T02:03:41.198947+00:00"},{"alias_kind":"arxiv_version","alias_value":"2008.09835v2","created_at":"2026-07-05T02:03:41.198947+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2008.09835","created_at":"2026-07-05T02:03:41.198947+00:00"},{"alias_kind":"pith_short_12","alias_value":"NFNIWPBH43UD","created_at":"2026-07-05T02:03:41.198947+00:00"},{"alias_kind":"pith_short_16","alias_value":"NFNIWPBH43UDJ6YH","created_at":"2026-07-05T02:03:41.198947+00:00"},{"alias_kind":"pith_short_8","alias_value":"NFNIWPBH","created_at":"2026-07-05T02:03:41.198947+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.23665","citing_title":"Radiative Mass Generation in Gauged Theories of Flavour: A Path to Fermion Mass Hierarchies","ref_index":113,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NFNIWPBH43UDJ6YHJUFMWK73AS","json":"https://pith.science/pith/NFNIWPBH43UDJ6YHJUFMWK73AS.json","graph_json":"https://pith.science/api/pith-number/NFNIWPBH43UDJ6YHJUFMWK73AS/graph.json","events_json":"https://pith.science/api/pith-number/NFNIWPBH43UDJ6YHJUFMWK73AS/events.json","paper":"https://pith.science/paper/NFNIWPBH"},"agent_actions":{"view_html":"https://pith.science/pith/NFNIWPBH43UDJ6YHJUFMWK73AS","download_json":"https://pith.science/pith/NFNIWPBH43UDJ6YHJUFMWK73AS.json","view_paper":"https://pith.science/paper/NFNIWPBH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2008.09835&json=true","fetch_graph":"https://pith.science/api/pith-number/NFNIWPBH43UDJ6YHJUFMWK73AS/graph.json","fetch_events":"https://pith.science/api/pith-number/NFNIWPBH43UDJ6YHJUFMWK73AS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NFNIWPBH43UDJ6YHJUFMWK73AS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NFNIWPBH43UDJ6YHJUFMWK73AS/action/storage_attestation","attest_author":"https://pith.science/pith/NFNIWPBH43UDJ6YHJUFMWK73AS/action/author_attestation","sign_citation":"https://pith.science/pith/NFNIWPBH43UDJ6YHJUFMWK73AS/action/citation_signature","submit_replication":"https://pith.science/pith/NFNIWPBH43UDJ6YHJUFMWK73AS/action/replication_record"}},"created_at":"2026-07-05T02:03:41.198947+00:00","updated_at":"2026-07-05T02:03:41.198947+00:00"}