{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:NSMWS3K6MLRI3FBFHHBUQUF7OC","short_pith_number":"pith:NSMWS3K6","schema_version":"1.0","canonical_sha256":"6c99696d5e62e28d942539c34850bf70bdf4ca5950ab17d251d256658f324faa","source":{"kind":"arxiv","id":"1109.4846","version":2},"attestation_state":"computed","paper":{"title":"Note on Higgs Decay into Two Photons $H\\to \\gamma\\gamma$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Da Huang, Yong Tang, Yue-Liang Wu","submitted_at":"2011-09-22T15:14:17Z","abstract_excerpt":"The Higgs decay $H\\to \\gamma\\gamma$ duo to the virtual $W$-loop effect is revisited in the unitary gauge by using the symmetry-preserving and divergent-behavior-preserving loop regularization method, which is realized in the four dimensional space-time without changing original theory. Though the one-loop amplitude of $H\\to \\gamma\\gamma$ is finite as the Higgs boson in the standard model has no direct interaction with the massless photons at tree level, while it involves both tensor-type and scalar-type divergent integrals which can in general destroy the gauge invariance without imposing a pr"},"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":"1109.4846","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-09-22T15:14:17Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"b81080a895d5895a22212771a8ec8b5e7fee5f7d3054827166191ae5d06c8654","abstract_canon_sha256":"956961aa25b2c4c278c935beeea8fc0928739aa56a34013a19cd0923e09a6990"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:58:12.584678Z","signature_b64":"MDRi27ZdS/sRjvVf5AKu7zigvidZCN9gbfncinXZIFmaWRhiOFlDUFldqgbYmwl80a99o/fVSaYPE9/mstWUCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6c99696d5e62e28d942539c34850bf70bdf4ca5950ab17d251d256658f324faa","last_reissued_at":"2026-05-18T03:58:12.584160Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:58:12.584160Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Note on Higgs Decay into Two Photons $H\\to \\gamma\\gamma$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Da Huang, Yong Tang, Yue-Liang Wu","submitted_at":"2011-09-22T15:14:17Z","abstract_excerpt":"The Higgs decay $H\\to \\gamma\\gamma$ duo to the virtual $W$-loop effect is revisited in the unitary gauge by using the symmetry-preserving and divergent-behavior-preserving loop regularization method, which is realized in the four dimensional space-time without changing original theory. Though the one-loop amplitude of $H\\to \\gamma\\gamma$ is finite as the Higgs boson in the standard model has no direct interaction with the massless photons at tree level, while it involves both tensor-type and scalar-type divergent integrals which can in general destroy the gauge invariance without imposing a pr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.4846","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":"1109.4846","created_at":"2026-05-18T03:58:12.584246+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.4846v2","created_at":"2026-05-18T03:58:12.584246+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.4846","created_at":"2026-05-18T03:58:12.584246+00:00"},{"alias_kind":"pith_short_12","alias_value":"NSMWS3K6MLRI","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_16","alias_value":"NSMWS3K6MLRI3FBF","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_8","alias_value":"NSMWS3K6","created_at":"2026-05-18T12:26:37.096874+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/NSMWS3K6MLRI3FBFHHBUQUF7OC","json":"https://pith.science/pith/NSMWS3K6MLRI3FBFHHBUQUF7OC.json","graph_json":"https://pith.science/api/pith-number/NSMWS3K6MLRI3FBFHHBUQUF7OC/graph.json","events_json":"https://pith.science/api/pith-number/NSMWS3K6MLRI3FBFHHBUQUF7OC/events.json","paper":"https://pith.science/paper/NSMWS3K6"},"agent_actions":{"view_html":"https://pith.science/pith/NSMWS3K6MLRI3FBFHHBUQUF7OC","download_json":"https://pith.science/pith/NSMWS3K6MLRI3FBFHHBUQUF7OC.json","view_paper":"https://pith.science/paper/NSMWS3K6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.4846&json=true","fetch_graph":"https://pith.science/api/pith-number/NSMWS3K6MLRI3FBFHHBUQUF7OC/graph.json","fetch_events":"https://pith.science/api/pith-number/NSMWS3K6MLRI3FBFHHBUQUF7OC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NSMWS3K6MLRI3FBFHHBUQUF7OC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NSMWS3K6MLRI3FBFHHBUQUF7OC/action/storage_attestation","attest_author":"https://pith.science/pith/NSMWS3K6MLRI3FBFHHBUQUF7OC/action/author_attestation","sign_citation":"https://pith.science/pith/NSMWS3K6MLRI3FBFHHBUQUF7OC/action/citation_signature","submit_replication":"https://pith.science/pith/NSMWS3K6MLRI3FBFHHBUQUF7OC/action/replication_record"}},"created_at":"2026-05-18T03:58:12.584246+00:00","updated_at":"2026-05-18T03:58:12.584246+00:00"}