{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:OQO2QWAMX2DF2XHCDMOSVOHURE","short_pith_number":"pith:OQO2QWAM","schema_version":"1.0","canonical_sha256":"741da8580cbe865d5ce21b1d2ab8f48926085ef35180ae40f04784f416f9cf02","source":{"kind":"arxiv","id":"2605.28590","version":1},"attestation_state":"computed","paper":{"title":"Two-loop QCD corrections to $ H \\rightarrow b + \\bar{b} + g $ at higher powers in the dimensional regulator","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chinmoy Dey, M. C. Kumar, Pulak Banerjee, Vaibhav Pandey, V. Ravindran","submitted_at":"2026-05-27T15:11:08Z","abstract_excerpt":"We compute the two-loop massless QCD corrections to the amplitude of Higgs boson decay to bottom quark pair and a gluon ($H \\rightarrow b + \\bar{b} + g$) in the higher powers of the dimensional regularization parameter $\\epsilon$. The calculation is performed by projecting the amplitude onto the appropriate Lorentz structures related to the process. We also show the numerical behaviour of the form factors for a few sample phase-space points. These amplitudes are necessary ingredients for computing the three-loop virtual corrections to bottom-quark annihilation to Higgs plus jet production at t"},"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":"2605.28590","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-05-27T15:11:08Z","cross_cats_sorted":[],"title_canon_sha256":"ca5c370285dc66d28bac460d603208aa64d895a4dfcfb1631fc202f9d744dadd","abstract_canon_sha256":"1dca314b135df687b9b9016bdf972dbfeb20be3a116f4e179dc3feafae636fbe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-28T02:04:57.238303Z","signature_b64":"e3HL9OS6w0/nTPjp9hzDnNo6q6cPimrP47cOWU13k91d/71Hdn7mxbjGSgFCTZd8hA4jmYRQvY5H9jZSHQ8oCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"741da8580cbe865d5ce21b1d2ab8f48926085ef35180ae40f04784f416f9cf02","last_reissued_at":"2026-05-28T02:04:57.237881Z","signature_status":"signed_v1","first_computed_at":"2026-05-28T02:04:57.237881Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two-loop QCD corrections to $ H \\rightarrow b + \\bar{b} + g $ at higher powers in the dimensional regulator","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chinmoy Dey, M. C. Kumar, Pulak Banerjee, Vaibhav Pandey, V. Ravindran","submitted_at":"2026-05-27T15:11:08Z","abstract_excerpt":"We compute the two-loop massless QCD corrections to the amplitude of Higgs boson decay to bottom quark pair and a gluon ($H \\rightarrow b + \\bar{b} + g$) in the higher powers of the dimensional regularization parameter $\\epsilon$. The calculation is performed by projecting the amplitude onto the appropriate Lorentz structures related to the process. We also show the numerical behaviour of the form factors for a few sample phase-space points. These amplitudes are necessary ingredients for computing the three-loop virtual corrections to bottom-quark annihilation to Higgs plus jet production at t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.28590","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/2605.28590/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":"2605.28590","created_at":"2026-05-28T02:04:57.237948+00:00"},{"alias_kind":"arxiv_version","alias_value":"2605.28590v1","created_at":"2026-05-28T02:04:57.237948+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.28590","created_at":"2026-05-28T02:04:57.237948+00:00"},{"alias_kind":"pith_short_12","alias_value":"OQO2QWAMX2DF","created_at":"2026-05-28T02:04:57.237948+00:00"},{"alias_kind":"pith_short_16","alias_value":"OQO2QWAMX2DF2XHC","created_at":"2026-05-28T02:04:57.237948+00:00"},{"alias_kind":"pith_short_8","alias_value":"OQO2QWAM","created_at":"2026-05-28T02:04:57.237948+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/OQO2QWAMX2DF2XHCDMOSVOHURE","json":"https://pith.science/pith/OQO2QWAMX2DF2XHCDMOSVOHURE.json","graph_json":"https://pith.science/api/pith-number/OQO2QWAMX2DF2XHCDMOSVOHURE/graph.json","events_json":"https://pith.science/api/pith-number/OQO2QWAMX2DF2XHCDMOSVOHURE/events.json","paper":"https://pith.science/paper/OQO2QWAM"},"agent_actions":{"view_html":"https://pith.science/pith/OQO2QWAMX2DF2XHCDMOSVOHURE","download_json":"https://pith.science/pith/OQO2QWAMX2DF2XHCDMOSVOHURE.json","view_paper":"https://pith.science/paper/OQO2QWAM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2605.28590&json=true","fetch_graph":"https://pith.science/api/pith-number/OQO2QWAMX2DF2XHCDMOSVOHURE/graph.json","fetch_events":"https://pith.science/api/pith-number/OQO2QWAMX2DF2XHCDMOSVOHURE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OQO2QWAMX2DF2XHCDMOSVOHURE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OQO2QWAMX2DF2XHCDMOSVOHURE/action/storage_attestation","attest_author":"https://pith.science/pith/OQO2QWAMX2DF2XHCDMOSVOHURE/action/author_attestation","sign_citation":"https://pith.science/pith/OQO2QWAMX2DF2XHCDMOSVOHURE/action/citation_signature","submit_replication":"https://pith.science/pith/OQO2QWAMX2DF2XHCDMOSVOHURE/action/replication_record"}},"created_at":"2026-05-28T02:04:57.237948+00:00","updated_at":"2026-05-28T02:04:57.237948+00:00"}