{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:Y7PAYSDJY57CC3LNJ3DI3DOC45","short_pith_number":"pith:Y7PAYSDJ","schema_version":"1.0","canonical_sha256":"c7de0c4869c77e216d6d4ec68d8dc2e74f285039ec427bdd47af5cdb5539e1c3","source":{"kind":"arxiv","id":"1808.01771","version":2},"attestation_state":"computed","paper":{"title":"Search for pair production of heavy vector-like quarks decaying into hadronic final states 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":"2018-08-06T08:34:52Z","abstract_excerpt":"A search is presented for the pair production of heavy vector-like quarks, $T\\bar T$ or $B\\bar B$, that decay into final states with jets and no reconstructed leptons. Jets in the final state are classified using a deep neural network as arising from hadronically decaying $W/Z$ bosons, Higgs bosons, top quarks, or background. The analysis uses data from the ATLAS experiment corresponding to 36.1 fb$^{-1}$ of proton-proton collisions with a center-of-mass energy of $\\sqrt{s} = 13$ TeV delivered by the Large Hadron Collider in 2015 and 2016. No significant deviation from the Standard Model expec"},"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":"1808.01771","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2018-08-06T08:34:52Z","cross_cats_sorted":[],"title_canon_sha256":"71fa4bd5e244999e8bf8c32b85c202c6ad3897065bb25acbd371a2abfe4ae60d","abstract_canon_sha256":"582c198feee2bb6dcd49d92f906a3e71ce1a95456c68b0ba6c77513172d0e94d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:01.566116Z","signature_b64":"qgyg1n6wXOgnGKOnPNgRoZWYK/FiAXJuAtojqwe8QrT7uh1V+EcH0Qp5gTasswyJtPYN1tNKo3KK/8RhMah8Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c7de0c4869c77e216d6d4ec68d8dc2e74f285039ec427bdd47af5cdb5539e1c3","last_reissued_at":"2026-05-17T23:59:01.565658Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:01.565658Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for pair production of heavy vector-like quarks decaying into hadronic final states 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":"2018-08-06T08:34:52Z","abstract_excerpt":"A search is presented for the pair production of heavy vector-like quarks, $T\\bar T$ or $B\\bar B$, that decay into final states with jets and no reconstructed leptons. Jets in the final state are classified using a deep neural network as arising from hadronically decaying $W/Z$ bosons, Higgs bosons, top quarks, or background. The analysis uses data from the ATLAS experiment corresponding to 36.1 fb$^{-1}$ of proton-proton collisions with a center-of-mass energy of $\\sqrt{s} = 13$ TeV delivered by the Large Hadron Collider in 2015 and 2016. No significant deviation from the Standard Model expec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.01771","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":""},"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":"1808.01771","created_at":"2026-05-17T23:59:01.565719+00:00"},{"alias_kind":"arxiv_version","alias_value":"1808.01771v2","created_at":"2026-05-17T23:59:01.565719+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.01771","created_at":"2026-05-17T23:59:01.565719+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y7PAYSDJY57C","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y7PAYSDJY57CC3LN","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y7PAYSDJ","created_at":"2026-05-18T12:33:04.347982+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.20848","citing_title":"Confronting Vector-Like Quark Models with LHC Searches","ref_index":59,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Y7PAYSDJY57CC3LNJ3DI3DOC45","json":"https://pith.science/pith/Y7PAYSDJY57CC3LNJ3DI3DOC45.json","graph_json":"https://pith.science/api/pith-number/Y7PAYSDJY57CC3LNJ3DI3DOC45/graph.json","events_json":"https://pith.science/api/pith-number/Y7PAYSDJY57CC3LNJ3DI3DOC45/events.json","paper":"https://pith.science/paper/Y7PAYSDJ"},"agent_actions":{"view_html":"https://pith.science/pith/Y7PAYSDJY57CC3LNJ3DI3DOC45","download_json":"https://pith.science/pith/Y7PAYSDJY57CC3LNJ3DI3DOC45.json","view_paper":"https://pith.science/paper/Y7PAYSDJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1808.01771&json=true","fetch_graph":"https://pith.science/api/pith-number/Y7PAYSDJY57CC3LNJ3DI3DOC45/graph.json","fetch_events":"https://pith.science/api/pith-number/Y7PAYSDJY57CC3LNJ3DI3DOC45/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y7PAYSDJY57CC3LNJ3DI3DOC45/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y7PAYSDJY57CC3LNJ3DI3DOC45/action/storage_attestation","attest_author":"https://pith.science/pith/Y7PAYSDJY57CC3LNJ3DI3DOC45/action/author_attestation","sign_citation":"https://pith.science/pith/Y7PAYSDJY57CC3LNJ3DI3DOC45/action/citation_signature","submit_replication":"https://pith.science/pith/Y7PAYSDJY57CC3LNJ3DI3DOC45/action/replication_record"}},"created_at":"2026-05-17T23:59:01.565719+00:00","updated_at":"2026-05-17T23:59:01.565719+00:00"}