{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:WEDVLXSBOHNPDHIYGYX2S3UIOG","short_pith_number":"pith:WEDVLXSB","schema_version":"1.0","canonical_sha256":"b10755de4171daf19d18362fa96e88719dce2909d0b62a078590de2e4f34e0bc","source":{"kind":"arxiv","id":"0808.0087","version":1},"attestation_state":"computed","paper":{"title":"MSSM Higgs Couplings to Bottom Quarks: Two-Loop Corrections","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David Noth, Michael Spira","submitted_at":"2008-08-01T10:26:39Z","abstract_excerpt":"We present the two-loop SUSY-QCD corrections to the effective bottom Yukawa couplings within the minimal supersymmetric extension of the Standard Model. The effective Yukawa couplings include the resummation of the non-decoupling corrections Delta m_b for large values of tg(beta). We have derived the two-loop SUSY-QCD corrections to the leading SUSY-QCD and top-induced SUSY-electroweak contributions to Delta m_b. The scale dependence of the resummed Yukawa couplings is reduced from O(10%) to the per-cent level. These results reduce the theoretical uncertainties of the MSSM Higgs branching rati"},"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":"0808.0087","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-08-01T10:26:39Z","cross_cats_sorted":[],"title_canon_sha256":"487c11b18eabf40278e9615349c3900078969be69194b35c0d85754625ac5d8d","abstract_canon_sha256":"5bc5af02651c5ff1df84dc920bffcdb6d1528834cd575530f47a6910250deb88"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:29:10.888268Z","signature_b64":"Z0pGgsV6PTpRkSOvidQCoG/TXvmpX/Vo0uTMgRncxhxho5axK66d/hSOB6awg/+aUU1FE0MybbBQE+9SfEpuAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b10755de4171daf19d18362fa96e88719dce2909d0b62a078590de2e4f34e0bc","last_reissued_at":"2026-07-04T15:29:10.887858Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:29:10.887858Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"MSSM Higgs Couplings to Bottom Quarks: Two-Loop Corrections","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David Noth, Michael Spira","submitted_at":"2008-08-01T10:26:39Z","abstract_excerpt":"We present the two-loop SUSY-QCD corrections to the effective bottom Yukawa couplings within the minimal supersymmetric extension of the Standard Model. The effective Yukawa couplings include the resummation of the non-decoupling corrections Delta m_b for large values of tg(beta). We have derived the two-loop SUSY-QCD corrections to the leading SUSY-QCD and top-induced SUSY-electroweak contributions to Delta m_b. The scale dependence of the resummed Yukawa couplings is reduced from O(10%) to the per-cent level. These results reduce the theoretical uncertainties of the MSSM Higgs branching rati"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0808.0087","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/0808.0087/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":"0808.0087","created_at":"2026-07-04T15:29:10.887925+00:00"},{"alias_kind":"arxiv_version","alias_value":"0808.0087v1","created_at":"2026-07-04T15:29:10.887925+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0808.0087","created_at":"2026-07-04T15:29:10.887925+00:00"},{"alias_kind":"pith_short_12","alias_value":"WEDVLXSBOHNP","created_at":"2026-07-04T15:29:10.887925+00:00"},{"alias_kind":"pith_short_16","alias_value":"WEDVLXSBOHNPDHIY","created_at":"2026-07-04T15:29:10.887925+00:00"},{"alias_kind":"pith_short_8","alias_value":"WEDVLXSB","created_at":"2026-07-04T15:29:10.887925+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.00931","citing_title":"Light Neutral Higgs-Boson Production at $e^+e^-$ Colliders in the Complex MSSM and NMSSM: A Full One-Loop Analysis","ref_index":33,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WEDVLXSBOHNPDHIYGYX2S3UIOG","json":"https://pith.science/pith/WEDVLXSBOHNPDHIYGYX2S3UIOG.json","graph_json":"https://pith.science/api/pith-number/WEDVLXSBOHNPDHIYGYX2S3UIOG/graph.json","events_json":"https://pith.science/api/pith-number/WEDVLXSBOHNPDHIYGYX2S3UIOG/events.json","paper":"https://pith.science/paper/WEDVLXSB"},"agent_actions":{"view_html":"https://pith.science/pith/WEDVLXSBOHNPDHIYGYX2S3UIOG","download_json":"https://pith.science/pith/WEDVLXSBOHNPDHIYGYX2S3UIOG.json","view_paper":"https://pith.science/paper/WEDVLXSB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0808.0087&json=true","fetch_graph":"https://pith.science/api/pith-number/WEDVLXSBOHNPDHIYGYX2S3UIOG/graph.json","fetch_events":"https://pith.science/api/pith-number/WEDVLXSBOHNPDHIYGYX2S3UIOG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WEDVLXSBOHNPDHIYGYX2S3UIOG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WEDVLXSBOHNPDHIYGYX2S3UIOG/action/storage_attestation","attest_author":"https://pith.science/pith/WEDVLXSBOHNPDHIYGYX2S3UIOG/action/author_attestation","sign_citation":"https://pith.science/pith/WEDVLXSBOHNPDHIYGYX2S3UIOG/action/citation_signature","submit_replication":"https://pith.science/pith/WEDVLXSBOHNPDHIYGYX2S3UIOG/action/replication_record"}},"created_at":"2026-07-04T15:29:10.887925+00:00","updated_at":"2026-07-04T15:29:10.887925+00:00"}