{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:6LZEKMKSJMS2QQ2Q4FAXE7M2OA","short_pith_number":"pith:6LZEKMKS","schema_version":"1.0","canonical_sha256":"f2f24531524b25a84350e141727d9a701b93e90388ab648edd60b65129e2bdc3","source":{"kind":"arxiv","id":"2211.12155","version":1},"attestation_state":"computed","paper":{"title":"Axion Couplings in Gauged $U(1)'$ Extensions of the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexey Kivel, Felix Yu, Julien Laux","submitted_at":"2022-11-22T10:34:56Z","abstract_excerpt":"We explore the effective theory of an axion in a gauged baryon number symmetry extension of the Standard Model (SM), where the axion is realized from a Dine-Fischler-Srednicki-Zhitnitsky (DFSZ) model construction. Integrating out the anomalons realizes a pattern of effective Wilson coefficients reflecting the factorization between the anomalous Peccei-Quinn and gauged baryon number symmetries. We construct and analyze the chiral transformation invariance of the axion effective theory, accounting for possible flavor-violating axion couplings. We calculate and study the unique phenomenology of 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":"2211.12155","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-11-22T10:34:56Z","cross_cats_sorted":[],"title_canon_sha256":"4b416802630c20c53f8d80750582bbae1a6555278149eafcd62dcebe338c91a0","abstract_canon_sha256":"26a2db5d4815cc6ccc2c751a8c6e49cf7189e7ebdf437e20fe944b743b6a8954"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:58:00.733234Z","signature_b64":"+Uwi9ZBPJ2wgqxMNFk1K7YHRtyl3VNnbIBRpIYCrp1ilnoOOQ42UIwXh7UCbNyN4UqZG6CsPgQtHnEUWDG3nCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2f24531524b25a84350e141727d9a701b93e90388ab648edd60b65129e2bdc3","last_reissued_at":"2026-07-05T05:58:00.732753Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:58:00.732753Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Axion Couplings in Gauged $U(1)'$ Extensions of the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexey Kivel, Felix Yu, Julien Laux","submitted_at":"2022-11-22T10:34:56Z","abstract_excerpt":"We explore the effective theory of an axion in a gauged baryon number symmetry extension of the Standard Model (SM), where the axion is realized from a Dine-Fischler-Srednicki-Zhitnitsky (DFSZ) model construction. Integrating out the anomalons realizes a pattern of effective Wilson coefficients reflecting the factorization between the anomalous Peccei-Quinn and gauged baryon number symmetries. We construct and analyze the chiral transformation invariance of the axion effective theory, accounting for possible flavor-violating axion couplings. We calculate and study the unique phenomenology of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.12155","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/2211.12155/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":"2211.12155","created_at":"2026-07-05T05:58:00.732812+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.12155v1","created_at":"2026-07-05T05:58:00.732812+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.12155","created_at":"2026-07-05T05:58:00.732812+00:00"},{"alias_kind":"pith_short_12","alias_value":"6LZEKMKSJMS2","created_at":"2026-07-05T05:58:00.732812+00:00"},{"alias_kind":"pith_short_16","alias_value":"6LZEKMKSJMS2QQ2Q","created_at":"2026-07-05T05:58:00.732812+00:00"},{"alias_kind":"pith_short_8","alias_value":"6LZEKMKS","created_at":"2026-07-05T05:58:00.732812+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.06068","citing_title":"Quark-universal $U(1)$ breaking scalar at the LHC","ref_index":15,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6LZEKMKSJMS2QQ2Q4FAXE7M2OA","json":"https://pith.science/pith/6LZEKMKSJMS2QQ2Q4FAXE7M2OA.json","graph_json":"https://pith.science/api/pith-number/6LZEKMKSJMS2QQ2Q4FAXE7M2OA/graph.json","events_json":"https://pith.science/api/pith-number/6LZEKMKSJMS2QQ2Q4FAXE7M2OA/events.json","paper":"https://pith.science/paper/6LZEKMKS"},"agent_actions":{"view_html":"https://pith.science/pith/6LZEKMKSJMS2QQ2Q4FAXE7M2OA","download_json":"https://pith.science/pith/6LZEKMKSJMS2QQ2Q4FAXE7M2OA.json","view_paper":"https://pith.science/paper/6LZEKMKS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.12155&json=true","fetch_graph":"https://pith.science/api/pith-number/6LZEKMKSJMS2QQ2Q4FAXE7M2OA/graph.json","fetch_events":"https://pith.science/api/pith-number/6LZEKMKSJMS2QQ2Q4FAXE7M2OA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6LZEKMKSJMS2QQ2Q4FAXE7M2OA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6LZEKMKSJMS2QQ2Q4FAXE7M2OA/action/storage_attestation","attest_author":"https://pith.science/pith/6LZEKMKSJMS2QQ2Q4FAXE7M2OA/action/author_attestation","sign_citation":"https://pith.science/pith/6LZEKMKSJMS2QQ2Q4FAXE7M2OA/action/citation_signature","submit_replication":"https://pith.science/pith/6LZEKMKSJMS2QQ2Q4FAXE7M2OA/action/replication_record"}},"created_at":"2026-07-05T05:58:00.732812+00:00","updated_at":"2026-07-05T05:58:00.732812+00:00"}