{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:XK6GDG4DBUR7U22CLINJBYBD36","short_pith_number":"pith:XK6GDG4D","schema_version":"1.0","canonical_sha256":"babc619b830d23fa6b425a1a90e023df8cf3c2a20b54358368155fabcac37161","source":{"kind":"arxiv","id":"2002.12223","version":2},"attestation_state":"computed","paper":{"title":"Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\\sqrt{s}=13$ TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2020-02-27T16:12:42Z","abstract_excerpt":"A search for heavy neutral Higgs bosons is performed using the LHC Run 2 data, corresponding to an integrated luminosity of 139 fb$^{-1}$ of proton-proton collisions at $\\sqrt{s}=13$ TeV recorded with the ATLAS detector. The search for heavy resonances is performed over the mass range 0.2-2.5 TeV for the $\\tau^+\\tau^-$ decay with at least one $\\tau$-lepton decaying into final states with hadrons. The data are in good agreement with the background prediction of the Standard Model. In the $M_{h}^{125}$ scenario of the Minimal Supersymmetric Standard Model, values of $\\tan\\beta>8$ and $\\tan\\beta>"},"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":"2002.12223","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2020-02-27T16:12:42Z","cross_cats_sorted":[],"title_canon_sha256":"d2f3f7defc83199d3a2122c99518518a4faab3f48e63266611f81ab8eb2be6d3","abstract_canon_sha256":"1545ff78961142b78f764cc280b1562b370442d7593046030bdeccae0be74e96"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:35:44.991443Z","signature_b64":"GCQQym6VyNd/aYmmEPc7cOEbXApHfSO5JPgHS/vlVnZLkHvqKA6PnRjd1r6yjvmo4+dUKP/Pm+vH+RumSd7hAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"babc619b830d23fa6b425a1a90e023df8cf3c2a20b54358368155fabcac37161","last_reissued_at":"2026-07-05T01:35:44.990962Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:35:44.990962Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\\sqrt{s}=13$ TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2020-02-27T16:12:42Z","abstract_excerpt":"A search for heavy neutral Higgs bosons is performed using the LHC Run 2 data, corresponding to an integrated luminosity of 139 fb$^{-1}$ of proton-proton collisions at $\\sqrt{s}=13$ TeV recorded with the ATLAS detector. The search for heavy resonances is performed over the mass range 0.2-2.5 TeV for the $\\tau^+\\tau^-$ decay with at least one $\\tau$-lepton decaying into final states with hadrons. The data are in good agreement with the background prediction of the Standard Model. In the $M_{h}^{125}$ scenario of the Minimal Supersymmetric Standard Model, values of $\\tan\\beta>8$ and $\\tan\\beta>"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2002.12223","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/2002.12223/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":"2002.12223","created_at":"2026-07-05T01:35:44.991019+00:00"},{"alias_kind":"arxiv_version","alias_value":"2002.12223v2","created_at":"2026-07-05T01:35:44.991019+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2002.12223","created_at":"2026-07-05T01:35:44.991019+00:00"},{"alias_kind":"pith_short_12","alias_value":"XK6GDG4DBUR7","created_at":"2026-07-05T01:35:44.991019+00:00"},{"alias_kind":"pith_short_16","alias_value":"XK6GDG4DBUR7U22C","created_at":"2026-07-05T01:35:44.991019+00:00"},{"alias_kind":"pith_short_8","alias_value":"XK6GDG4D","created_at":"2026-07-05T01:35:44.991019+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.29289","citing_title":"Hiding in the Shadow of the Upsilon: Ditaus from a Light Pseudoscalar","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2507.08927","citing_title":"Deciphering compressed electroweakino excesses with MadAnalysis 5","ref_index":89,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XK6GDG4DBUR7U22CLINJBYBD36","json":"https://pith.science/pith/XK6GDG4DBUR7U22CLINJBYBD36.json","graph_json":"https://pith.science/api/pith-number/XK6GDG4DBUR7U22CLINJBYBD36/graph.json","events_json":"https://pith.science/api/pith-number/XK6GDG4DBUR7U22CLINJBYBD36/events.json","paper":"https://pith.science/paper/XK6GDG4D"},"agent_actions":{"view_html":"https://pith.science/pith/XK6GDG4DBUR7U22CLINJBYBD36","download_json":"https://pith.science/pith/XK6GDG4DBUR7U22CLINJBYBD36.json","view_paper":"https://pith.science/paper/XK6GDG4D","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2002.12223&json=true","fetch_graph":"https://pith.science/api/pith-number/XK6GDG4DBUR7U22CLINJBYBD36/graph.json","fetch_events":"https://pith.science/api/pith-number/XK6GDG4DBUR7U22CLINJBYBD36/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XK6GDG4DBUR7U22CLINJBYBD36/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XK6GDG4DBUR7U22CLINJBYBD36/action/storage_attestation","attest_author":"https://pith.science/pith/XK6GDG4DBUR7U22CLINJBYBD36/action/author_attestation","sign_citation":"https://pith.science/pith/XK6GDG4DBUR7U22CLINJBYBD36/action/citation_signature","submit_replication":"https://pith.science/pith/XK6GDG4DBUR7U22CLINJBYBD36/action/replication_record"}},"created_at":"2026-07-05T01:35:44.991019+00:00","updated_at":"2026-07-05T01:35:44.991019+00:00"}