{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:H4QPNGQFRFLISYQQ7FQFTCJXLP","short_pith_number":"pith:H4QPNGQF","schema_version":"1.0","canonical_sha256":"3f20f69a058956896210f9605989375bf29d27b19fde9ba74a60171121894fc6","source":{"kind":"arxiv","id":"2305.03401","version":2},"attestation_state":"computed","paper":{"title":"Search for single production of vector-like $T$ quarks decaying into $Ht$ or $Zt$ in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2023-05-05T09:55:09Z","abstract_excerpt":"This paper describes a search for the single production of an up-type vector-like quark ($T$) decaying as $T \\rightarrow Ht$ or $T \\rightarrow Zt$. The search utilises a dataset of $pp$ collisions at $\\sqrt{s}=13$ TeV collected with the ATLAS detector during the 2015-2018 data-taking period of the Large Hadron Collider, corresponding to an integrated luminosityof 139 fb$^{-1}$. Data are analysed in final states containing a single lepton with multiple jets and $b$-jets. The presence of boosted heavy resonances in the event is exploited to discriminate the signal from the Standard Model backgro"},"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":"2305.03401","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2023-05-05T09:55:09Z","cross_cats_sorted":[],"title_canon_sha256":"be677e4a32e2e96580c53e15e3b194adf7045e84d33e319addca19be10cae43c","abstract_canon_sha256":"4d63c9053fdaaa11f051210bd08f63fd594ff30d857735f524667cefbcc8374c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:40:14.105194Z","signature_b64":"yodI9h81/qzWhyUx6uMWNyjfErUryRggPlvYLo5TSQF+nWvHXSngTUbMoqlBEWL62xHns5Vl2zc9b9GaWvumBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3f20f69a058956896210f9605989375bf29d27b19fde9ba74a60171121894fc6","last_reissued_at":"2026-07-05T09:40:14.104734Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:40:14.104734Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for single production of vector-like $T$ quarks decaying into $Ht$ or $Zt$ in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2023-05-05T09:55:09Z","abstract_excerpt":"This paper describes a search for the single production of an up-type vector-like quark ($T$) decaying as $T \\rightarrow Ht$ or $T \\rightarrow Zt$. The search utilises a dataset of $pp$ collisions at $\\sqrt{s}=13$ TeV collected with the ATLAS detector during the 2015-2018 data-taking period of the Large Hadron Collider, corresponding to an integrated luminosityof 139 fb$^{-1}$. Data are analysed in final states containing a single lepton with multiple jets and $b$-jets. The presence of boosted heavy resonances in the event is exploited to discriminate the signal from the Standard Model backgro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.03401","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/2305.03401/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":"2305.03401","created_at":"2026-07-05T09:40:14.104789+00:00"},{"alias_kind":"arxiv_version","alias_value":"2305.03401v2","created_at":"2026-07-05T09:40:14.104789+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.03401","created_at":"2026-07-05T09:40:14.104789+00:00"},{"alias_kind":"pith_short_12","alias_value":"H4QPNGQFRFLI","created_at":"2026-07-05T09:40:14.104789+00:00"},{"alias_kind":"pith_short_16","alias_value":"H4QPNGQFRFLISYQQ","created_at":"2026-07-05T09:40:14.104789+00:00"},{"alias_kind":"pith_short_8","alias_value":"H4QPNGQF","created_at":"2026-07-05T09:40:14.104789+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.28538","citing_title":"Search for pair-produced vector-like $T$-quarks decaying into $Ht$ final states in the lepton-plus-jets channel in $pp$ collisions at $\\sqrt{s}$=13 TeV with the ATLAS detector","ref_index":88,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/H4QPNGQFRFLISYQQ7FQFTCJXLP","json":"https://pith.science/pith/H4QPNGQFRFLISYQQ7FQFTCJXLP.json","graph_json":"https://pith.science/api/pith-number/H4QPNGQFRFLISYQQ7FQFTCJXLP/graph.json","events_json":"https://pith.science/api/pith-number/H4QPNGQFRFLISYQQ7FQFTCJXLP/events.json","paper":"https://pith.science/paper/H4QPNGQF"},"agent_actions":{"view_html":"https://pith.science/pith/H4QPNGQFRFLISYQQ7FQFTCJXLP","download_json":"https://pith.science/pith/H4QPNGQFRFLISYQQ7FQFTCJXLP.json","view_paper":"https://pith.science/paper/H4QPNGQF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2305.03401&json=true","fetch_graph":"https://pith.science/api/pith-number/H4QPNGQFRFLISYQQ7FQFTCJXLP/graph.json","fetch_events":"https://pith.science/api/pith-number/H4QPNGQFRFLISYQQ7FQFTCJXLP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/H4QPNGQFRFLISYQQ7FQFTCJXLP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/H4QPNGQFRFLISYQQ7FQFTCJXLP/action/storage_attestation","attest_author":"https://pith.science/pith/H4QPNGQFRFLISYQQ7FQFTCJXLP/action/author_attestation","sign_citation":"https://pith.science/pith/H4QPNGQFRFLISYQQ7FQFTCJXLP/action/citation_signature","submit_replication":"https://pith.science/pith/H4QPNGQFRFLISYQQ7FQFTCJXLP/action/replication_record"}},"created_at":"2026-07-05T09:40:14.104789+00:00","updated_at":"2026-07-05T09:40:14.104789+00:00"}