{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:ZNTQCKIRJLOI7WED66NPHTHYSU","short_pith_number":"pith:ZNTQCKIR","schema_version":"1.0","canonical_sha256":"cb670129114adc8fd883f79af3ccf8953f6000d9d5e5680e253579528496aee1","source":{"kind":"arxiv","id":"2209.06197","version":2},"attestation_state":"computed","paper":{"title":"Search for exotic Higgs boson decays H $\\to$ $\\mathcal{A}\\mathcal{A}$ $\\to$ 4$\\gamma$ with events containing two merged diphotons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2022-09-13T17:51:44Z","abstract_excerpt":"We present the first direct search for exotic Higgs boson decays H $\\to$ $\\mathcal{A}\\mathcal{A}$, $\\mathcal{A}$ $\\to$ $\\gamma\\gamma$ in events with two photonlike objects. The hypothetical particle $\\mathcal{A}$ is a low-mass spin-0 particle decaying promptly to a merged diphoton reconstructed as a single photonlike object. We analyze the data collected by the CMS experiment at $\\sqrt{s}$ = 13 TeV corresponding to an integrated luminosity of 136 fb$^{-1}$. No excess above the estimated background is found. We set upper limits on the branching fraction $\\mathcal{B}$(H $\\to$ $\\mathcal{A}\\mathca"},"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":"2209.06197","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2022-09-13T17:51:44Z","cross_cats_sorted":[],"title_canon_sha256":"ec74d63b6a669fe92b796086fa38fabfcd5a0f4fc6b16b5fa038e68bd24b1b04","abstract_canon_sha256":"9de1b241996751959049b2731225790e25907d7d843df7b2eb66a8cc19516015"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:56:29.851967Z","signature_b64":"pH/WrDMnfmOy5HGwKYTFtrb+KfDEz8ZMFpMVZ8AMF4najVpY7ZPYijcXBY17qzLE7UcAHbthV0dOZZVwiWXSCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cb670129114adc8fd883f79af3ccf8953f6000d9d5e5680e253579528496aee1","last_reissued_at":"2026-07-05T06:56:29.851464Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:56:29.851464Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for exotic Higgs boson decays H $\\to$ $\\mathcal{A}\\mathcal{A}$ $\\to$ 4$\\gamma$ with events containing two merged diphotons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2022-09-13T17:51:44Z","abstract_excerpt":"We present the first direct search for exotic Higgs boson decays H $\\to$ $\\mathcal{A}\\mathcal{A}$, $\\mathcal{A}$ $\\to$ $\\gamma\\gamma$ in events with two photonlike objects. The hypothetical particle $\\mathcal{A}$ is a low-mass spin-0 particle decaying promptly to a merged diphoton reconstructed as a single photonlike object. We analyze the data collected by the CMS experiment at $\\sqrt{s}$ = 13 TeV corresponding to an integrated luminosity of 136 fb$^{-1}$. No excess above the estimated background is found. We set upper limits on the branching fraction $\\mathcal{B}$(H $\\to$ $\\mathcal{A}\\mathca"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.06197","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/2209.06197/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":"2209.06197","created_at":"2026-07-05T06:56:29.851527+00:00"},{"alias_kind":"arxiv_version","alias_value":"2209.06197v2","created_at":"2026-07-05T06:56:29.851527+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.06197","created_at":"2026-07-05T06:56:29.851527+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZNTQCKIRJLOI","created_at":"2026-07-05T06:56:29.851527+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZNTQCKIRJLOI7WED","created_at":"2026-07-05T06:56:29.851527+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZNTQCKIR","created_at":"2026-07-05T06:56:29.851527+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2503.05463","citing_title":"Search for Higgs boson exotic decays into Lorentz-boosted light bosons in the four-$\\tau$ final state at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":33,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZNTQCKIRJLOI7WED66NPHTHYSU","json":"https://pith.science/pith/ZNTQCKIRJLOI7WED66NPHTHYSU.json","graph_json":"https://pith.science/api/pith-number/ZNTQCKIRJLOI7WED66NPHTHYSU/graph.json","events_json":"https://pith.science/api/pith-number/ZNTQCKIRJLOI7WED66NPHTHYSU/events.json","paper":"https://pith.science/paper/ZNTQCKIR"},"agent_actions":{"view_html":"https://pith.science/pith/ZNTQCKIRJLOI7WED66NPHTHYSU","download_json":"https://pith.science/pith/ZNTQCKIRJLOI7WED66NPHTHYSU.json","view_paper":"https://pith.science/paper/ZNTQCKIR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2209.06197&json=true","fetch_graph":"https://pith.science/api/pith-number/ZNTQCKIRJLOI7WED66NPHTHYSU/graph.json","fetch_events":"https://pith.science/api/pith-number/ZNTQCKIRJLOI7WED66NPHTHYSU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZNTQCKIRJLOI7WED66NPHTHYSU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZNTQCKIRJLOI7WED66NPHTHYSU/action/storage_attestation","attest_author":"https://pith.science/pith/ZNTQCKIRJLOI7WED66NPHTHYSU/action/author_attestation","sign_citation":"https://pith.science/pith/ZNTQCKIRJLOI7WED66NPHTHYSU/action/citation_signature","submit_replication":"https://pith.science/pith/ZNTQCKIRJLOI7WED66NPHTHYSU/action/replication_record"}},"created_at":"2026-07-05T06:56:29.851527+00:00","updated_at":"2026-07-05T06:56:29.851527+00:00"}