{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:NNXRHRBZKTD3YZWGIXIZZGE4LD","short_pith_number":"pith:NNXRHRBZ","schema_version":"1.0","canonical_sha256":"6b6f13c43954c7bc66c645d19c989c58dc5796581164f2cde097e5247fb991a6","source":{"kind":"arxiv","id":"1212.5074","version":3},"attestation_state":"computed","paper":{"title":"Full 1-loop calculation of BR$(B_{s,d}^0\\to \\ell \\bar \\ell)$ in models beyond the MSSM with SARAH and SPheno","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. Staub, H. Dreiner, K. Nickel, W. Porod","submitted_at":"2012-12-20T14:59:24Z","abstract_excerpt":"We present the possibility of calculating the quark flavor changing neutral current decays $B_{s}^0\\to \\ell \\bar \\ell$ and $B_{d}^0\\to \\ell \\bar \\ell$ for a large variety of supersymmetric models. For this purpose, the complete one-loop calculation has been implemented in a generic form in the Mathematica package SARAH. This information is used by SARAH to generate Fortran source code for SPheno for a numerical evaluation of these processes in a given model. We comment also on the possibility to use this setup for non-supersymmetric models."},"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":"1212.5074","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-20T14:59:24Z","cross_cats_sorted":[],"title_canon_sha256":"febb4a4c4f32e69c460caab8dfe4abfc6130bce9a1014d1effa651cf772eedfc","abstract_canon_sha256":"d1836400c6d3d515114af1f207a5a6505d80b0aed8a575a3747330c61b66b1a1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:16:51.337978Z","signature_b64":"TqOmDlZhn2Yc8mC4PGu7B6h4wRm7LzcQM8iR+1dAjyphh4ekh8mBnzZ6/8PHFNy2hLwL+kq/d5HXV8I6YbFhCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6b6f13c43954c7bc66c645d19c989c58dc5796581164f2cde097e5247fb991a6","last_reissued_at":"2026-05-18T03:16:51.337202Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:16:51.337202Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Full 1-loop calculation of BR$(B_{s,d}^0\\to \\ell \\bar \\ell)$ in models beyond the MSSM with SARAH and SPheno","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. Staub, H. Dreiner, K. Nickel, W. Porod","submitted_at":"2012-12-20T14:59:24Z","abstract_excerpt":"We present the possibility of calculating the quark flavor changing neutral current decays $B_{s}^0\\to \\ell \\bar \\ell$ and $B_{d}^0\\to \\ell \\bar \\ell$ for a large variety of supersymmetric models. For this purpose, the complete one-loop calculation has been implemented in a generic form in the Mathematica package SARAH. This information is used by SARAH to generate Fortran source code for SPheno for a numerical evaluation of these processes in a given model. We comment also on the possibility to use this setup for non-supersymmetric models."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.5074","kind":"arxiv","version":3},"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":"1212.5074","created_at":"2026-05-18T03:16:51.337336+00:00"},{"alias_kind":"arxiv_version","alias_value":"1212.5074v3","created_at":"2026-05-18T03:16:51.337336+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.5074","created_at":"2026-05-18T03:16:51.337336+00:00"},{"alias_kind":"pith_short_12","alias_value":"NNXRHRBZKTD3","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_16","alias_value":"NNXRHRBZKTD3YZWG","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_8","alias_value":"NNXRHRBZ","created_at":"2026-05-18T12:27:16.716162+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/NNXRHRBZKTD3YZWGIXIZZGE4LD","json":"https://pith.science/pith/NNXRHRBZKTD3YZWGIXIZZGE4LD.json","graph_json":"https://pith.science/api/pith-number/NNXRHRBZKTD3YZWGIXIZZGE4LD/graph.json","events_json":"https://pith.science/api/pith-number/NNXRHRBZKTD3YZWGIXIZZGE4LD/events.json","paper":"https://pith.science/paper/NNXRHRBZ"},"agent_actions":{"view_html":"https://pith.science/pith/NNXRHRBZKTD3YZWGIXIZZGE4LD","download_json":"https://pith.science/pith/NNXRHRBZKTD3YZWGIXIZZGE4LD.json","view_paper":"https://pith.science/paper/NNXRHRBZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1212.5074&json=true","fetch_graph":"https://pith.science/api/pith-number/NNXRHRBZKTD3YZWGIXIZZGE4LD/graph.json","fetch_events":"https://pith.science/api/pith-number/NNXRHRBZKTD3YZWGIXIZZGE4LD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NNXRHRBZKTD3YZWGIXIZZGE4LD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NNXRHRBZKTD3YZWGIXIZZGE4LD/action/storage_attestation","attest_author":"https://pith.science/pith/NNXRHRBZKTD3YZWGIXIZZGE4LD/action/author_attestation","sign_citation":"https://pith.science/pith/NNXRHRBZKTD3YZWGIXIZZGE4LD/action/citation_signature","submit_replication":"https://pith.science/pith/NNXRHRBZKTD3YZWGIXIZZGE4LD/action/replication_record"}},"created_at":"2026-05-18T03:16:51.337336+00:00","updated_at":"2026-05-18T03:16:51.337336+00:00"}