{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:TPK4J4DEI32F27XCBRQALFFIF7","short_pith_number":"pith:TPK4J4DE","schema_version":"1.0","canonical_sha256":"9bd5c4f06446f45d7ee20c600594a82fe77256b73255f3ff8ff306f5d5fc95b6","source":{"kind":"arxiv","id":"0908.4404","version":2},"attestation_state":"computed","paper":{"title":"Chirally enhanced corrections to FCNC processes in the generic MSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andreas Crivellin, Ulrich Nierste","submitted_at":"2009-08-30T16:09:46Z","abstract_excerpt":"Chirally enhanced supersymmetric QCD corrections to FCNC processes are investigated in the framework of the MSSM with generic sources of flavor violation. These corrections arise from flavor-changing self-energy diagrams and can be absorbed into a finite renormalization of the squark-quark-gluino vertex. In this way enhanced two-loop and even three-loop diagrams can be efficiently included into a leading-order (LO) calculation. Our corrections substantially change the values of the parameters delta^{d,LL}_{23}, delta^{d,LR}_{23}, delta^{d,RL}_{23}, and delta^{d,RR}_{23} extracted from Br[B->X_"},"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":"0908.4404","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-08-30T16:09:46Z","cross_cats_sorted":[],"title_canon_sha256":"0f25135776835e5dd2efe985525dd04d61f78ac05e852e131bdae6c5981090e3","abstract_canon_sha256":"f5d608df456e70a84dd8a42170386670d8875778f2841264b93cef0e7240830d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:47.526207Z","signature_b64":"Td70EN3O1Lg4zu3B2V+LbDvqKRXNQyQDWJLPjqVDN8a5fBsRSd4tHipwnLKx8Y/0HuigDTLivHHtXbVbfyRDBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9bd5c4f06446f45d7ee20c600594a82fe77256b73255f3ff8ff306f5d5fc95b6","last_reissued_at":"2026-05-18T02:24:47.525470Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:47.525470Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chirally enhanced corrections to FCNC processes in the generic MSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andreas Crivellin, Ulrich Nierste","submitted_at":"2009-08-30T16:09:46Z","abstract_excerpt":"Chirally enhanced supersymmetric QCD corrections to FCNC processes are investigated in the framework of the MSSM with generic sources of flavor violation. These corrections arise from flavor-changing self-energy diagrams and can be absorbed into a finite renormalization of the squark-quark-gluino vertex. In this way enhanced two-loop and even three-loop diagrams can be efficiently included into a leading-order (LO) calculation. Our corrections substantially change the values of the parameters delta^{d,LL}_{23}, delta^{d,LR}_{23}, delta^{d,RL}_{23}, and delta^{d,RR}_{23} extracted from Br[B->X_"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.4404","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":"0908.4404","created_at":"2026-05-18T02:24:47.525611+00:00"},{"alias_kind":"arxiv_version","alias_value":"0908.4404v2","created_at":"2026-05-18T02:24:47.525611+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.4404","created_at":"2026-05-18T02:24:47.525611+00:00"},{"alias_kind":"pith_short_12","alias_value":"TPK4J4DEI32F","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"TPK4J4DEI32F27XC","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"TPK4J4DE","created_at":"2026-05-18T12:26:01.383474+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.24924","citing_title":"Forward backward CP asymmetry in $\\tau^- \\to K \\pi \\nu_{\\tau}$ in the Left-Right Inverse seesaw model","ref_index":78,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TPK4J4DEI32F27XCBRQALFFIF7","json":"https://pith.science/pith/TPK4J4DEI32F27XCBRQALFFIF7.json","graph_json":"https://pith.science/api/pith-number/TPK4J4DEI32F27XCBRQALFFIF7/graph.json","events_json":"https://pith.science/api/pith-number/TPK4J4DEI32F27XCBRQALFFIF7/events.json","paper":"https://pith.science/paper/TPK4J4DE"},"agent_actions":{"view_html":"https://pith.science/pith/TPK4J4DEI32F27XCBRQALFFIF7","download_json":"https://pith.science/pith/TPK4J4DEI32F27XCBRQALFFIF7.json","view_paper":"https://pith.science/paper/TPK4J4DE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0908.4404&json=true","fetch_graph":"https://pith.science/api/pith-number/TPK4J4DEI32F27XCBRQALFFIF7/graph.json","fetch_events":"https://pith.science/api/pith-number/TPK4J4DEI32F27XCBRQALFFIF7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TPK4J4DEI32F27XCBRQALFFIF7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TPK4J4DEI32F27XCBRQALFFIF7/action/storage_attestation","attest_author":"https://pith.science/pith/TPK4J4DEI32F27XCBRQALFFIF7/action/author_attestation","sign_citation":"https://pith.science/pith/TPK4J4DEI32F27XCBRQALFFIF7/action/citation_signature","submit_replication":"https://pith.science/pith/TPK4J4DEI32F27XCBRQALFFIF7/action/replication_record"}},"created_at":"2026-05-18T02:24:47.525611+00:00","updated_at":"2026-05-18T02:24:47.525611+00:00"}