{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:K4EK3JIQC4VTBE7AOMCMCQJY66","short_pith_number":"pith:K4EK3JIQ","schema_version":"1.0","canonical_sha256":"5708ada510172b3093e07304c14138f781e3c7886499a7455e62583000cddb75","source":{"kind":"arxiv","id":"2608.03369","version":1},"attestation_state":"computed","paper":{"title":"Measurement of the Higgs boson decay to a low-mass dilepton system and a photon in $pp$ collisions at $\\sqrt{s} =$ 13 and 13.6 TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2026-08-04T09:20:15Z","abstract_excerpt":"A measurement is presented for the Higgs boson decaying into a photon and a pair of electrons or muons with an invariant mass $m_{\\ell\\ell} <$ 30 GeV, using $pp$ collision data at $\\sqrt{s} =$ 13.6 TeV recorded by the ATLAS detector at the Large Hadron Collider during the years 2022-2024, corresponding to an integrated luminosity of 164 fb$^{-1}$. The best-fit value of the signal strength parameter, defined as the ratio of the observed signal yield to the one expected in the Standard Model, is measured to be $\\mu = 0.64^{+0.44}_{-0.39}$ compared with the expected value of $\\mu = 1.00^{+0.47}_{"},"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":"2608.03369","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-08-04T09:20:15Z","cross_cats_sorted":[],"title_canon_sha256":"30df7ce72157126bbf2e032498aec80e9d277e7538f708c41d981e7b4491cfd1","abstract_canon_sha256":"6c5ce606cf17def85f8b947cabd576256c6c24e41728c80d035c6e6b9a6cd95e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-05T01:35:37.761846Z","signature_b64":"sF194WEYQA2/QNALxIJg+Xg0wi/5DOwMWFC/iYGj6NealPqKkXu61l0NCTSLgLcF3BiglBetTnHBFtbB/LlOBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5708ada510172b3093e07304c14138f781e3c7886499a7455e62583000cddb75","last_reissued_at":"2026-08-05T01:35:37.760330Z","signature_status":"signed_v1","first_computed_at":"2026-08-05T01:35:37.760330Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the Higgs boson decay to a low-mass dilepton system and a photon in $pp$ collisions at $\\sqrt{s} =$ 13 and 13.6 TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2026-08-04T09:20:15Z","abstract_excerpt":"A measurement is presented for the Higgs boson decaying into a photon and a pair of electrons or muons with an invariant mass $m_{\\ell\\ell} <$ 30 GeV, using $pp$ collision data at $\\sqrt{s} =$ 13.6 TeV recorded by the ATLAS detector at the Large Hadron Collider during the years 2022-2024, corresponding to an integrated luminosity of 164 fb$^{-1}$. The best-fit value of the signal strength parameter, defined as the ratio of the observed signal yield to the one expected in the Standard Model, is measured to be $\\mu = 0.64^{+0.44}_{-0.39}$ compared with the expected value of $\\mu = 1.00^{+0.47}_{"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.03369","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/2608.03369/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":"2608.03369","created_at":"2026-08-05T01:35:37.760783+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.03369v1","created_at":"2026-08-05T01:35:37.760783+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.03369","created_at":"2026-08-05T01:35:37.760783+00:00"},{"alias_kind":"pith_short_12","alias_value":"K4EK3JIQC4VT","created_at":"2026-08-05T01:35:37.760783+00:00"},{"alias_kind":"pith_short_16","alias_value":"K4EK3JIQC4VTBE7A","created_at":"2026-08-05T01:35:37.760783+00:00"},{"alias_kind":"pith_short_8","alias_value":"K4EK3JIQ","created_at":"2026-08-05T01:35:37.760783+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/K4EK3JIQC4VTBE7AOMCMCQJY66","json":"https://pith.science/pith/K4EK3JIQC4VTBE7AOMCMCQJY66.json","graph_json":"https://pith.science/api/pith-number/K4EK3JIQC4VTBE7AOMCMCQJY66/graph.json","events_json":"https://pith.science/api/pith-number/K4EK3JIQC4VTBE7AOMCMCQJY66/events.json","paper":"https://pith.science/paper/K4EK3JIQ"},"agent_actions":{"view_html":"https://pith.science/pith/K4EK3JIQC4VTBE7AOMCMCQJY66","download_json":"https://pith.science/pith/K4EK3JIQC4VTBE7AOMCMCQJY66.json","view_paper":"https://pith.science/paper/K4EK3JIQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.03369&json=true","fetch_graph":"https://pith.science/api/pith-number/K4EK3JIQC4VTBE7AOMCMCQJY66/graph.json","fetch_events":"https://pith.science/api/pith-number/K4EK3JIQC4VTBE7AOMCMCQJY66/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K4EK3JIQC4VTBE7AOMCMCQJY66/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K4EK3JIQC4VTBE7AOMCMCQJY66/action/storage_attestation","attest_author":"https://pith.science/pith/K4EK3JIQC4VTBE7AOMCMCQJY66/action/author_attestation","sign_citation":"https://pith.science/pith/K4EK3JIQC4VTBE7AOMCMCQJY66/action/citation_signature","submit_replication":"https://pith.science/pith/K4EK3JIQC4VTBE7AOMCMCQJY66/action/replication_record"}},"created_at":"2026-08-05T01:35:37.760783+00:00","updated_at":"2026-08-05T01:35:37.760783+00:00"}