{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:FLE4XOBLBG5YK2RVBF53PRK5NL","short_pith_number":"pith:FLE4XOBL","schema_version":"1.0","canonical_sha256":"2ac9cbb82b09bb856a35097bb7c55d6adba4c68913a5de21df3c04fa0612ef91","source":{"kind":"arxiv","id":"2103.10045","version":1},"attestation_state":"computed","paper":{"title":"One-loop form factors for $H\\rightarrow \\gamma^*\\gamma^*$ in $R_{\\xi}$ gauge","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dzung Tri Tran, Khiem Hong Phan","submitted_at":"2021-03-18T06:43:44Z","abstract_excerpt":"In this paper, we present general one-loop form factors for $H\\rightarrow \\gamma^* \\gamma^*$ in $R_{\\xi}$ gauge, considering all cases of two on-shell, one on-shell and two off-shell for final photons. The calculations are performed in standard model and in arbitrary beyond the standard models which charged scalar particles may be exchanged in one-loop diagrams. Analytic results for the form factors are shown in general forms which are expressed in terms of the Passarino-Veltman functions. We also confirm the results in previous computations which are available for the case of two on-shell pho"},"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":"2103.10045","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-03-18T06:43:44Z","cross_cats_sorted":[],"title_canon_sha256":"0785cd59b4a9fc7204df6b4d116557e9f3aa41258d67d9301a534b88943f1d91","abstract_canon_sha256":"9f2893cb92ed96d9cbcc749e183585ee136f73c34f195f1be93d0169f0142aac"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:24:15.968225Z","signature_b64":"67kI9n27o/h57OeipTVL7lJphZqIjznYzYA22zTqJeQHWNnlDzGg8gg/4427GHZrfxglizl5HDig+r+JjiLNBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2ac9cbb82b09bb856a35097bb7c55d6adba4c68913a5de21df3c04fa0612ef91","last_reissued_at":"2026-07-05T02:24:15.967876Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:24:15.967876Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"One-loop form factors for $H\\rightarrow \\gamma^*\\gamma^*$ in $R_{\\xi}$ gauge","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dzung Tri Tran, Khiem Hong Phan","submitted_at":"2021-03-18T06:43:44Z","abstract_excerpt":"In this paper, we present general one-loop form factors for $H\\rightarrow \\gamma^* \\gamma^*$ in $R_{\\xi}$ gauge, considering all cases of two on-shell, one on-shell and two off-shell for final photons. The calculations are performed in standard model and in arbitrary beyond the standard models which charged scalar particles may be exchanged in one-loop diagrams. Analytic results for the form factors are shown in general forms which are expressed in terms of the Passarino-Veltman functions. We also confirm the results in previous computations which are available for the case of two on-shell pho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.10045","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/2103.10045/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":"2103.10045","created_at":"2026-07-05T02:24:15.967940+00:00"},{"alias_kind":"arxiv_version","alias_value":"2103.10045v1","created_at":"2026-07-05T02:24:15.967940+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.10045","created_at":"2026-07-05T02:24:15.967940+00:00"},{"alias_kind":"pith_short_12","alias_value":"FLE4XOBLBG5Y","created_at":"2026-07-05T02:24:15.967940+00:00"},{"alias_kind":"pith_short_16","alias_value":"FLE4XOBLBG5YK2RV","created_at":"2026-07-05T02:24:15.967940+00:00"},{"alias_kind":"pith_short_8","alias_value":"FLE4XOBL","created_at":"2026-07-05T02:24:15.967940+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/FLE4XOBLBG5YK2RVBF53PRK5NL","json":"https://pith.science/pith/FLE4XOBLBG5YK2RVBF53PRK5NL.json","graph_json":"https://pith.science/api/pith-number/FLE4XOBLBG5YK2RVBF53PRK5NL/graph.json","events_json":"https://pith.science/api/pith-number/FLE4XOBLBG5YK2RVBF53PRK5NL/events.json","paper":"https://pith.science/paper/FLE4XOBL"},"agent_actions":{"view_html":"https://pith.science/pith/FLE4XOBLBG5YK2RVBF53PRK5NL","download_json":"https://pith.science/pith/FLE4XOBLBG5YK2RVBF53PRK5NL.json","view_paper":"https://pith.science/paper/FLE4XOBL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2103.10045&json=true","fetch_graph":"https://pith.science/api/pith-number/FLE4XOBLBG5YK2RVBF53PRK5NL/graph.json","fetch_events":"https://pith.science/api/pith-number/FLE4XOBLBG5YK2RVBF53PRK5NL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FLE4XOBLBG5YK2RVBF53PRK5NL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FLE4XOBLBG5YK2RVBF53PRK5NL/action/storage_attestation","attest_author":"https://pith.science/pith/FLE4XOBLBG5YK2RVBF53PRK5NL/action/author_attestation","sign_citation":"https://pith.science/pith/FLE4XOBLBG5YK2RVBF53PRK5NL/action/citation_signature","submit_replication":"https://pith.science/pith/FLE4XOBLBG5YK2RVBF53PRK5NL/action/replication_record"}},"created_at":"2026-07-05T02:24:15.967940+00:00","updated_at":"2026-07-05T02:24:15.967940+00:00"}