{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:AOJV2OZOPD4HRETLAFUIP23AEO","short_pith_number":"pith:AOJV2OZO","schema_version":"1.0","canonical_sha256":"03935d3b2e78f878926b016887eb6023ac37044ba13709e904d8d896c1164d02","source":{"kind":"arxiv","id":"1811.09179","version":1},"attestation_state":"computed","paper":{"title":"Properties of the decay $H\\to\\gamma\\gamma$ using the approximate $\\alpha_s^4$-corrections and the principle of maximum conformality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jian-Ming Shen, Jun Zeng, Qing Yu, Sheng-Quan Wang, Xing-Gang Wu, Xu-Dong Huang","submitted_at":"2018-11-22T14:07:35Z","abstract_excerpt":"The Higgs boson decay channel, $H\\to\\gamma\\gamma$, is one of the most important channels for probing the properties of the Higgs boson. In the paper, we reanalyze its decay width by using the QCD corrections up to $\\alpha_s^4$-order level. The principle of maximum conformality has been adopted to achieve a precise pQCD prediction without conventional renormalization scheme-and-scale ambiguities. By taking the Higgs mass as the one given by the ATLAS and CMS collaborations, i.e. $M_{H}=125.09\\pm0.21\\pm0.11$ GeV, we obtain $\\Gamma(H\\to \\gamma\\gamma)|_{\\rm LHC}=9.364^{+0.076}_{-0.075}$ KeV."},"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":"1811.09179","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-11-22T14:07:35Z","cross_cats_sorted":[],"title_canon_sha256":"ea13cf0a8ab6fa39264501c1d5147547c25576c06b83265a4c9d7202f0efc753","abstract_canon_sha256":"d3ce40d3e1975e3349e89050afc7a4cedd848fe58e983436f164029bfa0f173b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:39:41.548029Z","signature_b64":"77Ds+VNElWrWb2Tl/CEkfx3Izq21nFM83J3+uNuznXJp8fBVegQNA+EAZISOnSvXkYYUqOj5uyTwll7rSwukAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03935d3b2e78f878926b016887eb6023ac37044ba13709e904d8d896c1164d02","last_reissued_at":"2026-05-17T23:39:41.547602Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:39:41.547602Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Properties of the decay $H\\to\\gamma\\gamma$ using the approximate $\\alpha_s^4$-corrections and the principle of maximum conformality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jian-Ming Shen, Jun Zeng, Qing Yu, Sheng-Quan Wang, Xing-Gang Wu, Xu-Dong Huang","submitted_at":"2018-11-22T14:07:35Z","abstract_excerpt":"The Higgs boson decay channel, $H\\to\\gamma\\gamma$, is one of the most important channels for probing the properties of the Higgs boson. In the paper, we reanalyze its decay width by using the QCD corrections up to $\\alpha_s^4$-order level. The principle of maximum conformality has been adopted to achieve a precise pQCD prediction without conventional renormalization scheme-and-scale ambiguities. By taking the Higgs mass as the one given by the ATLAS and CMS collaborations, i.e. $M_{H}=125.09\\pm0.21\\pm0.11$ GeV, we obtain $\\Gamma(H\\to \\gamma\\gamma)|_{\\rm LHC}=9.364^{+0.076}_{-0.075}$ KeV."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.09179","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":""},"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":"1811.09179","created_at":"2026-05-17T23:39:41.547668+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.09179v1","created_at":"2026-05-17T23:39:41.547668+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.09179","created_at":"2026-05-17T23:39:41.547668+00:00"},{"alias_kind":"pith_short_12","alias_value":"AOJV2OZOPD4H","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_16","alias_value":"AOJV2OZOPD4HRETL","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_8","alias_value":"AOJV2OZO","created_at":"2026-05-18T12:32:13.499390+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/AOJV2OZOPD4HRETLAFUIP23AEO","json":"https://pith.science/pith/AOJV2OZOPD4HRETLAFUIP23AEO.json","graph_json":"https://pith.science/api/pith-number/AOJV2OZOPD4HRETLAFUIP23AEO/graph.json","events_json":"https://pith.science/api/pith-number/AOJV2OZOPD4HRETLAFUIP23AEO/events.json","paper":"https://pith.science/paper/AOJV2OZO"},"agent_actions":{"view_html":"https://pith.science/pith/AOJV2OZOPD4HRETLAFUIP23AEO","download_json":"https://pith.science/pith/AOJV2OZOPD4HRETLAFUIP23AEO.json","view_paper":"https://pith.science/paper/AOJV2OZO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.09179&json=true","fetch_graph":"https://pith.science/api/pith-number/AOJV2OZOPD4HRETLAFUIP23AEO/graph.json","fetch_events":"https://pith.science/api/pith-number/AOJV2OZOPD4HRETLAFUIP23AEO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AOJV2OZOPD4HRETLAFUIP23AEO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AOJV2OZOPD4HRETLAFUIP23AEO/action/storage_attestation","attest_author":"https://pith.science/pith/AOJV2OZOPD4HRETLAFUIP23AEO/action/author_attestation","sign_citation":"https://pith.science/pith/AOJV2OZOPD4HRETLAFUIP23AEO/action/citation_signature","submit_replication":"https://pith.science/pith/AOJV2OZOPD4HRETLAFUIP23AEO/action/replication_record"}},"created_at":"2026-05-17T23:39:41.547668+00:00","updated_at":"2026-05-17T23:39:41.547668+00:00"}