{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:GKOFSC45S4O574UIMWU2XWATM6","short_pith_number":"pith:GKOFSC45","schema_version":"1.0","canonical_sha256":"329c590b9d971ddff28865a9abd81367a5af607898ea13914ec59800dd30f34c","source":{"kind":"arxiv","id":"2207.00348","version":2},"attestation_state":"computed","paper":{"title":"Measurement of the properties of Higgs boson production at $\\sqrt{s} = 13$ TeV in the $H\\to\\gamma\\gamma$ channel using $139$ fb$^{-1}$ of $pp$ collision data 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":"2022-07-01T11:27:20Z","abstract_excerpt":"Measurements of Higgs boson production cross-sections are carried out in the diphoton decay channel using 139 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s} = 13$ TeV collected by the ATLAS experiment at the LHC. The analysis is based on the definition of 101 distinct signal regions using machine-learning techniques. The inclusive Higgs boson signal strength in the diphoton channel is measured to be $1.04^{+0.10}_{-0.09}$. Cross-sections for gluon-gluon fusion, vector-boson fusion, associated production with a $W$ or $Z$ boson, and top associated production processes are reported. An upper limi"},"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":"2207.00348","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2022-07-01T11:27:20Z","cross_cats_sorted":[],"title_canon_sha256":"0f82a396adbad89ada8ecbf85cc43ff0ce3068a27be0a2c1a736d13610d59f72","abstract_canon_sha256":"7a4592c34c6ef659ce538f0bc84d1e306e44b22881e642f10d9e7cf04f1f2719"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:51:18.308392Z","signature_b64":"jdpGCktXBSPzPagglkA7Q1J24D1+BPqyyS1hpPF9ICORNylU9Jc8XD7ruIwi+zCHT7TbH1LIv0tbxJhLpHa2Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"329c590b9d971ddff28865a9abd81367a5af607898ea13914ec59800dd30f34c","last_reissued_at":"2026-07-05T06:51:18.307841Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:51:18.307841Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the properties of Higgs boson production at $\\sqrt{s} = 13$ TeV in the $H\\to\\gamma\\gamma$ channel using $139$ fb$^{-1}$ of $pp$ collision data 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":"2022-07-01T11:27:20Z","abstract_excerpt":"Measurements of Higgs boson production cross-sections are carried out in the diphoton decay channel using 139 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s} = 13$ TeV collected by the ATLAS experiment at the LHC. The analysis is based on the definition of 101 distinct signal regions using machine-learning techniques. The inclusive Higgs boson signal strength in the diphoton channel is measured to be $1.04^{+0.10}_{-0.09}$. Cross-sections for gluon-gluon fusion, vector-boson fusion, associated production with a $W$ or $Z$ boson, and top associated production processes are reported. An upper limi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.00348","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/2207.00348/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":"2207.00348","created_at":"2026-07-05T06:51:18.307908+00:00"},{"alias_kind":"arxiv_version","alias_value":"2207.00348v2","created_at":"2026-07-05T06:51:18.307908+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.00348","created_at":"2026-07-05T06:51:18.307908+00:00"},{"alias_kind":"pith_short_12","alias_value":"GKOFSC45S4O5","created_at":"2026-07-05T06:51:18.307908+00:00"},{"alias_kind":"pith_short_16","alias_value":"GKOFSC45S4O574UI","created_at":"2026-07-05T06:51:18.307908+00:00"},{"alias_kind":"pith_short_8","alias_value":"GKOFSC45","created_at":"2026-07-05T06:51:18.307908+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"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":26,"is_internal_anchor":false},{"citing_arxiv_id":"2412.10665","citing_title":"Pretrained Event Classification Model for High Energy Physics Analysis","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2507.03495","citing_title":"Study of Higgs boson pair production in the $HH \\rightarrow b \\overline{b} \\gamma \\gamma$ final state with 308 fb$^{-1}$ of data collected at $\\sqrt{s} =$ 13 TeV and 13.6 TeV by the ATLAS experiment","ref_index":92,"is_internal_anchor":false},{"citing_arxiv_id":"2511.04796","citing_title":"Interpretation of LHC excesses at 95 GeV and 152 GeV in an extended Georgi-Machacek model","ref_index":76,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21670","citing_title":"Effective field theory interpretation of ATLAS measurements involving the Higgs boson, electroweak bosons and the top quark","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GKOFSC45S4O574UIMWU2XWATM6","json":"https://pith.science/pith/GKOFSC45S4O574UIMWU2XWATM6.json","graph_json":"https://pith.science/api/pith-number/GKOFSC45S4O574UIMWU2XWATM6/graph.json","events_json":"https://pith.science/api/pith-number/GKOFSC45S4O574UIMWU2XWATM6/events.json","paper":"https://pith.science/paper/GKOFSC45"},"agent_actions":{"view_html":"https://pith.science/pith/GKOFSC45S4O574UIMWU2XWATM6","download_json":"https://pith.science/pith/GKOFSC45S4O574UIMWU2XWATM6.json","view_paper":"https://pith.science/paper/GKOFSC45","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2207.00348&json=true","fetch_graph":"https://pith.science/api/pith-number/GKOFSC45S4O574UIMWU2XWATM6/graph.json","fetch_events":"https://pith.science/api/pith-number/GKOFSC45S4O574UIMWU2XWATM6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GKOFSC45S4O574UIMWU2XWATM6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GKOFSC45S4O574UIMWU2XWATM6/action/storage_attestation","attest_author":"https://pith.science/pith/GKOFSC45S4O574UIMWU2XWATM6/action/author_attestation","sign_citation":"https://pith.science/pith/GKOFSC45S4O574UIMWU2XWATM6/action/citation_signature","submit_replication":"https://pith.science/pith/GKOFSC45S4O574UIMWU2XWATM6/action/replication_record"}},"created_at":"2026-07-05T06:51:18.307908+00:00","updated_at":"2026-07-05T06:51:18.307908+00:00"}