{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:BIGTPY3OBKRSF47F66I3DPGQ3X","short_pith_number":"pith:BIGTPY3O","schema_version":"1.0","canonical_sha256":"0a0d37e36e0aa322f3e5f791b1bcd0ddea52f6e447f075a256ea857699c9cb38","source":{"kind":"arxiv","id":"1408.7084","version":2},"attestation_state":"computed","paper":{"title":"Measurement of Higgs boson production in the diphoton decay channel in $pp$ collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2014-08-29T17:35:34Z","abstract_excerpt":"A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 5.4 fb$^{-1}$ of proton-proton collisions data at $\\sqrt{s}=7$ TeV and 20.3 fb$^{-1}$ at $\\sqrt{s}=8$ TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be $\\mu = 1.17 \\pm 0.27$ at the value of the Higgs boson mass measured by ATLAS, $m_{H}$ = 125.4 GeV. The analysis is optimized to measure the signal s"},"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":"1408.7084","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2014-08-29T17:35:34Z","cross_cats_sorted":[],"title_canon_sha256":"1f37d1794c92ba284035cb241d7cfa6301ed55d844051ce0e11e35bdc3486ace","abstract_canon_sha256":"83c3e26192dd081fb7a6bdfa25e1c3ada3493f5568b4382dc6bd5aa00d09bfb6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:30:17.661962Z","signature_b64":"oTcQt9s3pY6bqjYQaQnggHv78K4v4WHUBr4oXGyORon78wMaT7QaeNBXVtvdyz7EdHCfBsoPFdkeQpKd80j4CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0a0d37e36e0aa322f3e5f791b1bcd0ddea52f6e447f075a256ea857699c9cb38","last_reissued_at":"2026-05-18T02:30:17.661509Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:30:17.661509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of Higgs boson production in the diphoton decay channel in $pp$ collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2014-08-29T17:35:34Z","abstract_excerpt":"A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 5.4 fb$^{-1}$ of proton-proton collisions data at $\\sqrt{s}=7$ TeV and 20.3 fb$^{-1}$ at $\\sqrt{s}=8$ TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be $\\mu = 1.17 \\pm 0.27$ at the value of the Higgs boson mass measured by ATLAS, $m_{H}$ = 125.4 GeV. The analysis is optimized to measure the signal s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.7084","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":""},"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":"1408.7084","created_at":"2026-05-18T02:30:17.661566+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.7084v2","created_at":"2026-05-18T02:30:17.661566+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.7084","created_at":"2026-05-18T02:30:17.661566+00:00"},{"alias_kind":"pith_short_12","alias_value":"BIGTPY3OBKRS","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_16","alias_value":"BIGTPY3OBKRSF47F","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_8","alias_value":"BIGTPY3O","created_at":"2026-05-18T12:28:22.404517+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"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":97,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BIGTPY3OBKRSF47F66I3DPGQ3X","json":"https://pith.science/pith/BIGTPY3OBKRSF47F66I3DPGQ3X.json","graph_json":"https://pith.science/api/pith-number/BIGTPY3OBKRSF47F66I3DPGQ3X/graph.json","events_json":"https://pith.science/api/pith-number/BIGTPY3OBKRSF47F66I3DPGQ3X/events.json","paper":"https://pith.science/paper/BIGTPY3O"},"agent_actions":{"view_html":"https://pith.science/pith/BIGTPY3OBKRSF47F66I3DPGQ3X","download_json":"https://pith.science/pith/BIGTPY3OBKRSF47F66I3DPGQ3X.json","view_paper":"https://pith.science/paper/BIGTPY3O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.7084&json=true","fetch_graph":"https://pith.science/api/pith-number/BIGTPY3OBKRSF47F66I3DPGQ3X/graph.json","fetch_events":"https://pith.science/api/pith-number/BIGTPY3OBKRSF47F66I3DPGQ3X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BIGTPY3OBKRSF47F66I3DPGQ3X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BIGTPY3OBKRSF47F66I3DPGQ3X/action/storage_attestation","attest_author":"https://pith.science/pith/BIGTPY3OBKRSF47F66I3DPGQ3X/action/author_attestation","sign_citation":"https://pith.science/pith/BIGTPY3OBKRSF47F66I3DPGQ3X/action/citation_signature","submit_replication":"https://pith.science/pith/BIGTPY3OBKRSF47F66I3DPGQ3X/action/replication_record"}},"created_at":"2026-05-18T02:30:17.661566+00:00","updated_at":"2026-05-18T02:30:17.661566+00:00"}