{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:SMMHW4USD2DOLFYYNJT3DKYV63","short_pith_number":"pith:SMMHW4US","schema_version":"1.0","canonical_sha256":"93187b72921e86e597186a67b1ab15f6ce0fc61e5327c7dd8621a92cdd570699","source":{"kind":"arxiv","id":"1706.08510","version":3},"attestation_state":"computed","paper":{"title":"$B$ decay anomalies from nonabelian local horizontal symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"James M. Cline, Jorge Martin Camalich","submitted_at":"2017-06-26T17:59:50Z","abstract_excerpt":"Recent anomalies in $B\\to K^{(*)}\\ell\\ell$ meson decays are consistent with exchange of a heavy $Z'$ vector boson. Here we try to connect such new physics to understanding the origin of flavor, by gauging generation number. Phenomenological and theoretical considerations suggest that the smallest viable flavor symmetry (not including any extra U(1) factors) is chiral ${\\rm SU(3)}_L\\times{\\rm SU(3)}_R$, which acts only on generation indices and does not distinguish between quarks and leptons. Spontaneous breaking of the symmetry gives rise to the standard model Yukawa matrices, and masses for 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":"1706.08510","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-06-26T17:59:50Z","cross_cats_sorted":[],"title_canon_sha256":"b8c010942d14702dcc44caa7f5c15b1cf587847c2f4f6604ae6c19f924848700","abstract_canon_sha256":"39db4c4ab43b6e5a1a74475e1bcb0a617aba4c23846fa29288856e2dea4351b7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:59.537436Z","signature_b64":"VcXvy2LJO5o1KFIffbqRELFRl8QsIyAtC6XDJnZJeXAc8qsvYhdzhbVSHYdD9ieEiQNJR5ZJabojwUrGRjGBAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"93187b72921e86e597186a67b1ab15f6ce0fc61e5327c7dd8621a92cdd570699","last_reissued_at":"2026-05-18T00:32:59.536894Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:59.536894Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$B$ decay anomalies from nonabelian local horizontal symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"James M. Cline, Jorge Martin Camalich","submitted_at":"2017-06-26T17:59:50Z","abstract_excerpt":"Recent anomalies in $B\\to K^{(*)}\\ell\\ell$ meson decays are consistent with exchange of a heavy $Z'$ vector boson. Here we try to connect such new physics to understanding the origin of flavor, by gauging generation number. Phenomenological and theoretical considerations suggest that the smallest viable flavor symmetry (not including any extra U(1) factors) is chiral ${\\rm SU(3)}_L\\times{\\rm SU(3)}_R$, which acts only on generation indices and does not distinguish between quarks and leptons. Spontaneous breaking of the symmetry gives rise to the standard model Yukawa matrices, and masses for t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.08510","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":"1706.08510","created_at":"2026-05-18T00:32:59.536978+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.08510v3","created_at":"2026-05-18T00:32:59.536978+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.08510","created_at":"2026-05-18T00:32:59.536978+00:00"},{"alias_kind":"pith_short_12","alias_value":"SMMHW4USD2DO","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_16","alias_value":"SMMHW4USD2DOLFYY","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_8","alias_value":"SMMHW4US","created_at":"2026-05-18T12:31:43.269735+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/SMMHW4USD2DOLFYYNJT3DKYV63","json":"https://pith.science/pith/SMMHW4USD2DOLFYYNJT3DKYV63.json","graph_json":"https://pith.science/api/pith-number/SMMHW4USD2DOLFYYNJT3DKYV63/graph.json","events_json":"https://pith.science/api/pith-number/SMMHW4USD2DOLFYYNJT3DKYV63/events.json","paper":"https://pith.science/paper/SMMHW4US"},"agent_actions":{"view_html":"https://pith.science/pith/SMMHW4USD2DOLFYYNJT3DKYV63","download_json":"https://pith.science/pith/SMMHW4USD2DOLFYYNJT3DKYV63.json","view_paper":"https://pith.science/paper/SMMHW4US","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.08510&json=true","fetch_graph":"https://pith.science/api/pith-number/SMMHW4USD2DOLFYYNJT3DKYV63/graph.json","fetch_events":"https://pith.science/api/pith-number/SMMHW4USD2DOLFYYNJT3DKYV63/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SMMHW4USD2DOLFYYNJT3DKYV63/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SMMHW4USD2DOLFYYNJT3DKYV63/action/storage_attestation","attest_author":"https://pith.science/pith/SMMHW4USD2DOLFYYNJT3DKYV63/action/author_attestation","sign_citation":"https://pith.science/pith/SMMHW4USD2DOLFYYNJT3DKYV63/action/citation_signature","submit_replication":"https://pith.science/pith/SMMHW4USD2DOLFYYNJT3DKYV63/action/replication_record"}},"created_at":"2026-05-18T00:32:59.536978+00:00","updated_at":"2026-05-18T00:32:59.536978+00:00"}