{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:YRZOQW7DM2NHWBEAG6DDHZO4YL","short_pith_number":"pith:YRZOQW7D","schema_version":"1.0","canonical_sha256":"c472e85be3669a7b0480378633e5dcc2c8b7b98696ed5ffb19169e71f4b5d8f3","source":{"kind":"arxiv","id":"2412.17584","version":2},"attestation_state":"computed","paper":{"title":"Search for charged Higgs bosons produced in top-quark decays or in association with top quarks and decaying via $H^{\\pm} \\to \\tau^{\\pm}\\nu_{\\tau}$ in 13 TeV $pp$ collisions 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":"2024-12-23T13:57:57Z","abstract_excerpt":"Charged Higgs bosons produced either in top-quark decays or in association with a top-quark, subsequently decaying via $H^{\\pm} \\to \\tau^{\\pm}\\nu_{\\tau}$, are searched for in 140 $\\text{fb}^{-1}$ of proton-proton collision data at $\\sqrt{s}=13$ TeV recorded with the ATLAS detector. Depending on whether the top-quark produced together with the $H^{\\pm}$ decays hadronically or semi-leptonically, the search targets $\\tau$+jets or $\\tau$+lepton final states, in both cases with a $\\tau$-lepton decaying into a neutrino and hadrons. No significant excess over the Standard Model background expectation"},"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":"2412.17584","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2024-12-23T13:57:57Z","cross_cats_sorted":[],"title_canon_sha256":"b282ee3c25a03b5ecab7d96b18788e595890a82f0047fc8a8553bfc67c8f40cf","abstract_canon_sha256":"033fb65732763d685e39df2fc65c2c7fdf658de1bb05915e1b4b09218a4c6bde"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:18:40.956803Z","signature_b64":"OpbcYQ0H+SQJVuwgYlgGZxlejZYAneM6jEmMo8icBTJKzZFO0TSDoDLsKvb66x+b7XpBczD2ArDcDMgTEgHnDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c472e85be3669a7b0480378633e5dcc2c8b7b98696ed5ffb19169e71f4b5d8f3","last_reissued_at":"2026-07-05T11:18:40.956367Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:18:40.956367Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for charged Higgs bosons produced in top-quark decays or in association with top quarks and decaying via $H^{\\pm} \\to \\tau^{\\pm}\\nu_{\\tau}$ in 13 TeV $pp$ collisions 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":"2024-12-23T13:57:57Z","abstract_excerpt":"Charged Higgs bosons produced either in top-quark decays or in association with a top-quark, subsequently decaying via $H^{\\pm} \\to \\tau^{\\pm}\\nu_{\\tau}$, are searched for in 140 $\\text{fb}^{-1}$ of proton-proton collision data at $\\sqrt{s}=13$ TeV recorded with the ATLAS detector. Depending on whether the top-quark produced together with the $H^{\\pm}$ decays hadronically or semi-leptonically, the search targets $\\tau$+jets or $\\tau$+lepton final states, in both cases with a $\\tau$-lepton decaying into a neutrino and hadrons. No significant excess over the Standard Model background expectation"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.17584","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/2412.17584/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":"2412.17584","created_at":"2026-07-05T11:18:40.956422+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.17584v2","created_at":"2026-07-05T11:18:40.956422+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.17584","created_at":"2026-07-05T11:18:40.956422+00:00"},{"alias_kind":"pith_short_12","alias_value":"YRZOQW7DM2NH","created_at":"2026-07-05T11:18:40.956422+00:00"},{"alias_kind":"pith_short_16","alias_value":"YRZOQW7DM2NHWBEA","created_at":"2026-07-05T11:18:40.956422+00:00"},{"alias_kind":"pith_short_8","alias_value":"YRZOQW7D","created_at":"2026-07-05T11:18:40.956422+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"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":30,"is_internal_anchor":false},{"citing_arxiv_id":"2509.07094","citing_title":"Searching for a Charged Higgs Boson in Top-Quark Decays via the $WZ$ Mode","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04233","citing_title":"Indications for New Higgs Bosons","ref_index":43,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YRZOQW7DM2NHWBEAG6DDHZO4YL","json":"https://pith.science/pith/YRZOQW7DM2NHWBEAG6DDHZO4YL.json","graph_json":"https://pith.science/api/pith-number/YRZOQW7DM2NHWBEAG6DDHZO4YL/graph.json","events_json":"https://pith.science/api/pith-number/YRZOQW7DM2NHWBEAG6DDHZO4YL/events.json","paper":"https://pith.science/paper/YRZOQW7D"},"agent_actions":{"view_html":"https://pith.science/pith/YRZOQW7DM2NHWBEAG6DDHZO4YL","download_json":"https://pith.science/pith/YRZOQW7DM2NHWBEAG6DDHZO4YL.json","view_paper":"https://pith.science/paper/YRZOQW7D","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.17584&json=true","fetch_graph":"https://pith.science/api/pith-number/YRZOQW7DM2NHWBEAG6DDHZO4YL/graph.json","fetch_events":"https://pith.science/api/pith-number/YRZOQW7DM2NHWBEAG6DDHZO4YL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YRZOQW7DM2NHWBEAG6DDHZO4YL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YRZOQW7DM2NHWBEAG6DDHZO4YL/action/storage_attestation","attest_author":"https://pith.science/pith/YRZOQW7DM2NHWBEAG6DDHZO4YL/action/author_attestation","sign_citation":"https://pith.science/pith/YRZOQW7DM2NHWBEAG6DDHZO4YL/action/citation_signature","submit_replication":"https://pith.science/pith/YRZOQW7DM2NHWBEAG6DDHZO4YL/action/replication_record"}},"created_at":"2026-07-05T11:18:40.956422+00:00","updated_at":"2026-07-05T11:18:40.956422+00:00"}