{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:JID4GSHZ4OVUDUDGJNQQKCPVRR","short_pith_number":"pith:JID4GSHZ","schema_version":"1.0","canonical_sha256":"4a07c348f9e3ab41d0664b610509f58c6a6a1d455056a8eb6b536b6bfd0eb7b9","source":{"kind":"arxiv","id":"1909.02845","version":2},"attestation_state":"computed","paper":{"title":"Combined measurements of Higgs boson production and decay using up to $80$ fb$^{-1}$ of proton-proton collision data at $\\sqrt{s}=$ 13 TeV collected 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":"2019-09-06T12:16:38Z","abstract_excerpt":"Combined measurements of Higgs boson production cross sections and branching fractions are presented. The combination is based on the analyses of the Higgs boson decay modes $H \\to \\gamma\\gamma$, $ZZ^\\ast$, $WW^\\ast$, $\\tau\\tau$, $b\\bar{b}$, $\\mu\\mu$, searches for decays into invisible final states, and on measurements of off-shell Higgs boson production. Up to $79.8$ fb$^{-1}$ of proton-proton collision data collected at $\\sqrt{s}=$ 13 TeV with the ATLAS detector are used. Results are presented for the gluon-gluon fusion and vector-boson fusion processes, and for associated production with ve"},"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":"1909.02845","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-09-06T12:16:38Z","cross_cats_sorted":[],"title_canon_sha256":"b3f4aa8f6c144df56c7ddfba41ca7f40081390e7bc47f2231260568a8b59699b","abstract_canon_sha256":"78a624ae79d94ee92eca920d3a6d067e38508a01a5574cdb392b182d6510c5d1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:39:38.309020Z","signature_b64":"VMEF0Tdzp5pLJxh1Veoj2Q5XJJnL+MVHglvqE5ynkWJwpl2QzfAbcGR86WZotK4aQhsxXEa2Uai6Xw/nJd2YDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a07c348f9e3ab41d0664b610509f58c6a6a1d455056a8eb6b536b6bfd0eb7b9","last_reissued_at":"2026-07-05T00:39:38.308605Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:39:38.308605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Combined measurements of Higgs boson production and decay using up to $80$ fb$^{-1}$ of proton-proton collision data at $\\sqrt{s}=$ 13 TeV collected 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":"2019-09-06T12:16:38Z","abstract_excerpt":"Combined measurements of Higgs boson production cross sections and branching fractions are presented. The combination is based on the analyses of the Higgs boson decay modes $H \\to \\gamma\\gamma$, $ZZ^\\ast$, $WW^\\ast$, $\\tau\\tau$, $b\\bar{b}$, $\\mu\\mu$, searches for decays into invisible final states, and on measurements of off-shell Higgs boson production. Up to $79.8$ fb$^{-1}$ of proton-proton collision data collected at $\\sqrt{s}=$ 13 TeV with the ATLAS detector are used. Results are presented for the gluon-gluon fusion and vector-boson fusion processes, and for associated production with ve"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1909.02845","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/1909.02845/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":"1909.02845","created_at":"2026-07-05T00:39:38.308662+00:00"},{"alias_kind":"arxiv_version","alias_value":"1909.02845v2","created_at":"2026-07-05T00:39:38.308662+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1909.02845","created_at":"2026-07-05T00:39:38.308662+00:00"},{"alias_kind":"pith_short_12","alias_value":"JID4GSHZ4OVU","created_at":"2026-07-05T00:39:38.308662+00:00"},{"alias_kind":"pith_short_16","alias_value":"JID4GSHZ4OVUDUDG","created_at":"2026-07-05T00:39:38.308662+00:00"},{"alias_kind":"pith_short_8","alias_value":"JID4GSHZ","created_at":"2026-07-05T00:39:38.308662+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.04855","citing_title":"Probing the Higgs-top Yukawa interaction in the $t\\bar{t}H$ and $tH$ processes using $H\\rightarrow\\gamma\\gamma$ with the ATLAS detector","ref_index":3,"is_internal_anchor":false},{"citing_arxiv_id":"2605.15270","citing_title":"Light states in real 3HDMs with spontaneous CP violation and softly broken symmetries","ref_index":50,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JID4GSHZ4OVUDUDGJNQQKCPVRR","json":"https://pith.science/pith/JID4GSHZ4OVUDUDGJNQQKCPVRR.json","graph_json":"https://pith.science/api/pith-number/JID4GSHZ4OVUDUDGJNQQKCPVRR/graph.json","events_json":"https://pith.science/api/pith-number/JID4GSHZ4OVUDUDGJNQQKCPVRR/events.json","paper":"https://pith.science/paper/JID4GSHZ"},"agent_actions":{"view_html":"https://pith.science/pith/JID4GSHZ4OVUDUDGJNQQKCPVRR","download_json":"https://pith.science/pith/JID4GSHZ4OVUDUDGJNQQKCPVRR.json","view_paper":"https://pith.science/paper/JID4GSHZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1909.02845&json=true","fetch_graph":"https://pith.science/api/pith-number/JID4GSHZ4OVUDUDGJNQQKCPVRR/graph.json","fetch_events":"https://pith.science/api/pith-number/JID4GSHZ4OVUDUDGJNQQKCPVRR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JID4GSHZ4OVUDUDGJNQQKCPVRR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JID4GSHZ4OVUDUDGJNQQKCPVRR/action/storage_attestation","attest_author":"https://pith.science/pith/JID4GSHZ4OVUDUDGJNQQKCPVRR/action/author_attestation","sign_citation":"https://pith.science/pith/JID4GSHZ4OVUDUDGJNQQKCPVRR/action/citation_signature","submit_replication":"https://pith.science/pith/JID4GSHZ4OVUDUDGJNQQKCPVRR/action/replication_record"}},"created_at":"2026-07-05T00:39:38.308662+00:00","updated_at":"2026-07-05T00:39:38.308662+00:00"}