{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:S7O6V6I552UXNKHT335TZLUY6A","short_pith_number":"pith:S7O6V6I5","schema_version":"1.0","canonical_sha256":"97ddeaf91deea976a8f3defb3cae98f0162c4a5b823ad47a42cd7cce8fc9a93c","source":{"kind":"arxiv","id":"1712.08895","version":2},"attestation_state":"computed","paper":{"title":"Search for the Standard Model Higgs boson produced in association with top quarks and decaying into a $b\\bar{b}$ pair 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":"2017-12-24T09:22:58Z","abstract_excerpt":"A search for the Standard Model Higgs boson produced in association with a top-quark pair, $t\\bar{t}H$, is presented. The analysis uses 36.1 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s}$ = 13 TeV, collected with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. The search targets the $H \\to b\\bar{b}$ decay mode. The selected events contain either one or two electrons or muons from the top-quark decays, and are then categorized according to the number of jets and how likely these are to contain $b$-hadrons. Multivariate techniques are used to discriminate between signal and bac"},"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":"1712.08895","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2017-12-24T09:22:58Z","cross_cats_sorted":[],"title_canon_sha256":"f35eca4b599b7123ddfe2df8c699de8cfbb94fa3e65b114c3ee77b58c767b74f","abstract_canon_sha256":"9cf4c45abe476f979becf985ee1a91af314e46335695a21020ec123d5d270370"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:16:08.114949Z","signature_b64":"TuKmmJZqjKvutgneuDKJKO4K8LwekMCLfaQp9DBbXmuIXZkT3uWh0vz5ffehw4VJJCt61PsT4cn1aADfp4A3Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"97ddeaf91deea976a8f3defb3cae98f0162c4a5b823ad47a42cd7cce8fc9a93c","last_reissued_at":"2026-05-18T00:16:08.114354Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:16:08.114354Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for the Standard Model Higgs boson produced in association with top quarks and decaying into a $b\\bar{b}$ pair 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":"2017-12-24T09:22:58Z","abstract_excerpt":"A search for the Standard Model Higgs boson produced in association with a top-quark pair, $t\\bar{t}H$, is presented. The analysis uses 36.1 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s}$ = 13 TeV, collected with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. The search targets the $H \\to b\\bar{b}$ decay mode. The selected events contain either one or two electrons or muons from the top-quark decays, and are then categorized according to the number of jets and how likely these are to contain $b$-hadrons. Multivariate techniques are used to discriminate between signal and bac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.08895","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":"1712.08895","created_at":"2026-05-18T00:16:08.114467+00:00"},{"alias_kind":"arxiv_version","alias_value":"1712.08895v2","created_at":"2026-05-18T00:16:08.114467+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.08895","created_at":"2026-05-18T00:16:08.114467+00:00"},{"alias_kind":"pith_short_12","alias_value":"S7O6V6I552UX","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_16","alias_value":"S7O6V6I552UXNKHT","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_8","alias_value":"S7O6V6I5","created_at":"2026-05-18T12:31:43.269735+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"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":105,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":136,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":136,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/S7O6V6I552UXNKHT335TZLUY6A","json":"https://pith.science/pith/S7O6V6I552UXNKHT335TZLUY6A.json","graph_json":"https://pith.science/api/pith-number/S7O6V6I552UXNKHT335TZLUY6A/graph.json","events_json":"https://pith.science/api/pith-number/S7O6V6I552UXNKHT335TZLUY6A/events.json","paper":"https://pith.science/paper/S7O6V6I5"},"agent_actions":{"view_html":"https://pith.science/pith/S7O6V6I552UXNKHT335TZLUY6A","download_json":"https://pith.science/pith/S7O6V6I552UXNKHT335TZLUY6A.json","view_paper":"https://pith.science/paper/S7O6V6I5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1712.08895&json=true","fetch_graph":"https://pith.science/api/pith-number/S7O6V6I552UXNKHT335TZLUY6A/graph.json","fetch_events":"https://pith.science/api/pith-number/S7O6V6I552UXNKHT335TZLUY6A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/S7O6V6I552UXNKHT335TZLUY6A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/S7O6V6I552UXNKHT335TZLUY6A/action/storage_attestation","attest_author":"https://pith.science/pith/S7O6V6I552UXNKHT335TZLUY6A/action/author_attestation","sign_citation":"https://pith.science/pith/S7O6V6I552UXNKHT335TZLUY6A/action/citation_signature","submit_replication":"https://pith.science/pith/S7O6V6I552UXNKHT335TZLUY6A/action/replication_record"}},"created_at":"2026-05-18T00:16:08.114467+00:00","updated_at":"2026-05-18T00:16:08.114467+00:00"}