{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV","short_pith_number":"pith:HSBEVQJ2","schema_version":"1.0","canonical_sha256":"3c824ac13acc649f9d1fe961ccf42dcd5653358887b02c2ffd6fd77aa770decb","source":{"kind":"arxiv","id":"2607.22193","version":1},"attestation_state":"computed","paper":{"title":"Cross-section measurements of boosted Higgs boson production in final states with pairs of hadronically decaying $\\tau$-leptons with the ATLAS experiment","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2026-07-24T11:07:48Z","abstract_excerpt":"Cross section measurements of high-Lorentz boosted Higgs boson production in final states with pairs of hadronically decaying $\\tau$-leptons are presented. The analysis is based on the full Run 2 data sample of proton-proton collisions at a centre-of-mass energy of $\\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of 140 $\\mathrm{fb}^{-1}$, and a partial Run 3 data sample at $\\sqrt{s} = 13.6$ TeV with an integrated luminosity of 162 $\\mathrm{fb}^{-1}$ collected in 2022-2024 with the ATLAS experiment. The analysis extends the sensitivity of previous $H \\to \\tau\\tau$ measurements to"},"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":"2607.22193","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-07-24T11:07:48Z","cross_cats_sorted":[],"title_canon_sha256":"093465563fc3b373375090ce08361ec81dc4452b74c292cd12f8145a0dc5d177","abstract_canon_sha256":"be5a875bbfaa0d6f401b4415d9ef7c167e5146c372a6bb3c6d340fe7e4e46c75"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-27T01:20:53.278118Z","signature_b64":"u9w/qlzZob7Yhf85NADT4EagF3Zj02aWH2NAuDxQRlXFe4qXHzPz6nwG/adPMfT9ekmaWEv1EXXsHeTTz1HOAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c824ac13acc649f9d1fe961ccf42dcd5653358887b02c2ffd6fd77aa770decb","last_reissued_at":"2026-07-27T01:20:53.277278Z","signature_status":"signed_v1","first_computed_at":"2026-07-27T01:20:53.277278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Cross-section measurements of boosted Higgs boson production in final states with pairs of hadronically decaying $\\tau$-leptons with the ATLAS experiment","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2026-07-24T11:07:48Z","abstract_excerpt":"Cross section measurements of high-Lorentz boosted Higgs boson production in final states with pairs of hadronically decaying $\\tau$-leptons are presented. The analysis is based on the full Run 2 data sample of proton-proton collisions at a centre-of-mass energy of $\\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of 140 $\\mathrm{fb}^{-1}$, and a partial Run 3 data sample at $\\sqrt{s} = 13.6$ TeV with an integrated luminosity of 162 $\\mathrm{fb}^{-1}$ collected in 2022-2024 with the ATLAS experiment. The analysis extends the sensitivity of previous $H \\to \\tau\\tau$ measurements to"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.22193","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.22193/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":"2607.22193","created_at":"2026-07-27T01:20:53.277712+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.22193v1","created_at":"2026-07-27T01:20:53.277712+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.22193","created_at":"2026-07-27T01:20:53.277712+00:00"},{"alias_kind":"pith_short_12","alias_value":"HSBEVQJ2ZRSJ","created_at":"2026-07-27T01:20:53.277712+00:00"},{"alias_kind":"pith_short_16","alias_value":"HSBEVQJ2ZRSJ7HI7","created_at":"2026-07-27T01:20:53.277712+00:00"},{"alias_kind":"pith_short_8","alias_value":"HSBEVQJ2","created_at":"2026-07-27T01:20:53.277712+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV","json":"https://pith.science/pith/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV.json","graph_json":"https://pith.science/api/pith-number/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV/graph.json","events_json":"https://pith.science/api/pith-number/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV/events.json","paper":"https://pith.science/paper/HSBEVQJ2"},"agent_actions":{"view_html":"https://pith.science/pith/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV","download_json":"https://pith.science/pith/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV.json","view_paper":"https://pith.science/paper/HSBEVQJ2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.22193&json=true","fetch_graph":"https://pith.science/api/pith-number/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV/graph.json","fetch_events":"https://pith.science/api/pith-number/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV/action/storage_attestation","attest_author":"https://pith.science/pith/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV/action/author_attestation","sign_citation":"https://pith.science/pith/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV/action/citation_signature","submit_replication":"https://pith.science/pith/HSBEVQJ2ZRSJ7HI75FQ4Z5BNZV/action/replication_record"}},"created_at":"2026-07-27T01:20:53.277712+00:00","updated_at":"2026-07-27T01:20:53.277712+00:00"}