{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:QHUNZGKP4PHLECAGZPC7SS6WI4","short_pith_number":"pith:QHUNZGKP","schema_version":"1.0","canonical_sha256":"81e8dc994fe3ceb20806cbc5f94bd6471354fe554b47ec0d48f1943582ca69bf","source":{"kind":"arxiv","id":"hep-ex/0508051","version":1},"attestation_state":"computed","paper":{"title":"Search for neutral MSSM Higgs bosons decaying to tau pairs in p-pbar collisions at sqrt(s)=1.96 TeV","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CDF Collaboration","submitted_at":"2005-08-25T18:58:34Z","abstract_excerpt":"We present a search for neutral supersymmetric Higgs bosons decaying to tau pairs produced in p-pbar collisions at sqrt(s) = 1.96 TeV. The data, corresponding to 310 pb^(-1) integrated luminosity, were collected with the CDF II detector at the Tevatron collider at Fermilab. No significant excess above the standard model backgrounds is observed. We set exclusion limits on the production cross section times branching fraction to tau pairs for Higgs masses in the range from 90 to 250 GeV/c^2."},"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":"hep-ex/0508051","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2005-08-25T18:58:34Z","cross_cats_sorted":[],"title_canon_sha256":"19b1b925539738ef62424a6a614008a5412705d6d8724ac18ad1f5ef77c49001","abstract_canon_sha256":"dcfa51b527fd0a0e2d340f6113390c74b246b8b8ed82f2267d8839ae2f3979cb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:30.329311Z","signature_b64":"86W1SMmck9OMbIrLImSXApZENspuXyCjqJ4q68bIsXYLAo3JyP73N9mZCh9hQdKvvP7UJCnkane4mMWpG9INCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"81e8dc994fe3ceb20806cbc5f94bd6471354fe554b47ec0d48f1943582ca69bf","last_reissued_at":"2026-05-18T03:47:30.328845Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:30.328845Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for neutral MSSM Higgs bosons decaying to tau pairs in p-pbar collisions at sqrt(s)=1.96 TeV","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CDF Collaboration","submitted_at":"2005-08-25T18:58:34Z","abstract_excerpt":"We present a search for neutral supersymmetric Higgs bosons decaying to tau pairs produced in p-pbar collisions at sqrt(s) = 1.96 TeV. The data, corresponding to 310 pb^(-1) integrated luminosity, were collected with the CDF II detector at the Tevatron collider at Fermilab. No significant excess above the standard model backgrounds is observed. We set exclusion limits on the production cross section times branching fraction to tau pairs for Higgs masses in the range from 90 to 250 GeV/c^2."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0508051","kind":"arxiv","version":1},"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":"hep-ex/0508051","created_at":"2026-05-18T03:47:30.328913+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0508051v1","created_at":"2026-05-18T03:47:30.328913+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0508051","created_at":"2026-05-18T03:47:30.328913+00:00"},{"alias_kind":"pith_short_12","alias_value":"QHUNZGKP4PHL","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_16","alias_value":"QHUNZGKP4PHLECAG","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_8","alias_value":"QHUNZGKP","created_at":"2026-05-18T12:25:53.335082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.25103","citing_title":"Search for low-mass resonances decaying to $\\tau\\tau$ and measurement of the $\\Upsilon$ $\\to$ $\\tau\\tau$ decay in proton-proton collisions at $\\sqrt{s}$ = 13.6 TeV","ref_index":52,"is_internal_anchor":true},{"citing_arxiv_id":"2605.19144","citing_title":"Search for Higgs boson decays into two neutral scalars with unequal masses in final states with b quarks and tau leptons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":106,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QHUNZGKP4PHLECAGZPC7SS6WI4","json":"https://pith.science/pith/QHUNZGKP4PHLECAGZPC7SS6WI4.json","graph_json":"https://pith.science/api/pith-number/QHUNZGKP4PHLECAGZPC7SS6WI4/graph.json","events_json":"https://pith.science/api/pith-number/QHUNZGKP4PHLECAGZPC7SS6WI4/events.json","paper":"https://pith.science/paper/QHUNZGKP"},"agent_actions":{"view_html":"https://pith.science/pith/QHUNZGKP4PHLECAGZPC7SS6WI4","download_json":"https://pith.science/pith/QHUNZGKP4PHLECAGZPC7SS6WI4.json","view_paper":"https://pith.science/paper/QHUNZGKP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0508051&json=true","fetch_graph":"https://pith.science/api/pith-number/QHUNZGKP4PHLECAGZPC7SS6WI4/graph.json","fetch_events":"https://pith.science/api/pith-number/QHUNZGKP4PHLECAGZPC7SS6WI4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QHUNZGKP4PHLECAGZPC7SS6WI4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QHUNZGKP4PHLECAGZPC7SS6WI4/action/storage_attestation","attest_author":"https://pith.science/pith/QHUNZGKP4PHLECAGZPC7SS6WI4/action/author_attestation","sign_citation":"https://pith.science/pith/QHUNZGKP4PHLECAGZPC7SS6WI4/action/citation_signature","submit_replication":"https://pith.science/pith/QHUNZGKP4PHLECAGZPC7SS6WI4/action/replication_record"}},"created_at":"2026-05-18T03:47:30.328913+00:00","updated_at":"2026-05-18T03:47:30.328913+00:00"}