{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:VGXGJDAFT6OXWQ35GCX5YEJYZQ","short_pith_number":"pith:VGXGJDAF","schema_version":"1.0","canonical_sha256":"a9ae648c059f9d7b437d30afdc1138cc0564a7925e97db75b228e5397cf5ccf4","source":{"kind":"arxiv","id":"2209.10910","version":2},"attestation_state":"computed","paper":{"title":"Search for resonant and non-resonant Higgs boson pair production in the $b\\bar b\\tau^+\\tau^-$ decay channel using 13 TeV $pp$ collision data from the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2022-09-22T10:44:11Z","abstract_excerpt":"A search for Higgs boson pair production in events with two $b$-jets and two $\\tau$-leptons is presented, using a proton-proton collision dataset with an integrated luminosity of 139 fb$^{-1}$ collected at $\\sqrt{s}=13$ TeV by the ATLAS experiment at the LHC. Higgs boson pairs produced non-resonantly or in the decay of a narrow scalar resonance in the mass range from 251 to 1600 GeV are targeted. Events in which at least one $\\tau$-lepton decays hadronically are considered, and multivariate discriminants are used to reject the backgrounds. No significant excess of events above the expected 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":"2209.10910","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2022-09-22T10:44:11Z","cross_cats_sorted":[],"title_canon_sha256":"aafa48f53a1c89288010b1038b4e0deb4e765df6630401848e332d43098353f7","abstract_canon_sha256":"72b8044d7a10dfadcddee5b31d2a0ba4658e0468ccbd35610d6858b6c49a7d23"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:33:17.149973Z","signature_b64":"0KUn985u1IQGHPeGWDSjJOY83TbwwfibK2CnoqysQpMp0GVJtJ/i9UnawHuMWldEn1L1lyhcIpwA/FD6fbwFAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a9ae648c059f9d7b437d30afdc1138cc0564a7925e97db75b228e5397cf5ccf4","last_reissued_at":"2026-07-05T06:33:17.149509Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:33:17.149509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for resonant and non-resonant Higgs boson pair production in the $b\\bar b\\tau^+\\tau^-$ decay channel using 13 TeV $pp$ collision data from the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2022-09-22T10:44:11Z","abstract_excerpt":"A search for Higgs boson pair production in events with two $b$-jets and two $\\tau$-leptons is presented, using a proton-proton collision dataset with an integrated luminosity of 139 fb$^{-1}$ collected at $\\sqrt{s}=13$ TeV by the ATLAS experiment at the LHC. Higgs boson pairs produced non-resonantly or in the decay of a narrow scalar resonance in the mass range from 251 to 1600 GeV are targeted. Events in which at least one $\\tau$-lepton decays hadronically are considered, and multivariate discriminants are used to reject the backgrounds. No significant excess of events above the expected bac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.10910","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/2209.10910/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":"2209.10910","created_at":"2026-07-05T06:33:17.149565+00:00"},{"alias_kind":"arxiv_version","alias_value":"2209.10910v2","created_at":"2026-07-05T06:33:17.149565+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.10910","created_at":"2026-07-05T06:33:17.149565+00:00"},{"alias_kind":"pith_short_12","alias_value":"VGXGJDAFT6OX","created_at":"2026-07-05T06:33:17.149565+00:00"},{"alias_kind":"pith_short_16","alias_value":"VGXGJDAFT6OXWQ35","created_at":"2026-07-05T06:33:17.149565+00:00"},{"alias_kind":"pith_short_8","alias_value":"VGXGJDAF","created_at":"2026-07-05T06:33:17.149565+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.29345","citing_title":"Alignment and Enhanced Multi-Higgs Production","ref_index":25,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VGXGJDAFT6OXWQ35GCX5YEJYZQ","json":"https://pith.science/pith/VGXGJDAFT6OXWQ35GCX5YEJYZQ.json","graph_json":"https://pith.science/api/pith-number/VGXGJDAFT6OXWQ35GCX5YEJYZQ/graph.json","events_json":"https://pith.science/api/pith-number/VGXGJDAFT6OXWQ35GCX5YEJYZQ/events.json","paper":"https://pith.science/paper/VGXGJDAF"},"agent_actions":{"view_html":"https://pith.science/pith/VGXGJDAFT6OXWQ35GCX5YEJYZQ","download_json":"https://pith.science/pith/VGXGJDAFT6OXWQ35GCX5YEJYZQ.json","view_paper":"https://pith.science/paper/VGXGJDAF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2209.10910&json=true","fetch_graph":"https://pith.science/api/pith-number/VGXGJDAFT6OXWQ35GCX5YEJYZQ/graph.json","fetch_events":"https://pith.science/api/pith-number/VGXGJDAFT6OXWQ35GCX5YEJYZQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VGXGJDAFT6OXWQ35GCX5YEJYZQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VGXGJDAFT6OXWQ35GCX5YEJYZQ/action/storage_attestation","attest_author":"https://pith.science/pith/VGXGJDAFT6OXWQ35GCX5YEJYZQ/action/author_attestation","sign_citation":"https://pith.science/pith/VGXGJDAFT6OXWQ35GCX5YEJYZQ/action/citation_signature","submit_replication":"https://pith.science/pith/VGXGJDAFT6OXWQ35GCX5YEJYZQ/action/replication_record"}},"created_at":"2026-07-05T06:33:17.149565+00:00","updated_at":"2026-07-05T06:33:17.149565+00:00"}