{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:KTQLO3U3NNG5JJ62AOXU2LCF54","short_pith_number":"pith:KTQLO3U3","schema_version":"1.0","canonical_sha256":"54e0b76e9b6b4dd4a7da03af4d2c45ef2cb80a01ce3b5be58fd00e4587994058","source":{"kind":"arxiv","id":"2402.14059","version":2},"attestation_state":"computed","paper":{"title":"Visible GeV ALP from TeV Vector-like Leptons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arturo de Giorgi, Luca Merlo, Marta Fuentes Zamoro","submitted_at":"2024-02-21T19:00:01Z","abstract_excerpt":"We present a model where a GeV axion-like-particle (ALP) is predicted in a large portion of the parameter space due to the presence of explicit Peccei-Quinn symmetry-breaking terms in an exotic leptonic sector. The latter provides a solution to the muon $g-2$ anomaly, within the framework of the Linear Seesaw neutrino mechanism. The spectrum is extended by a complex scalar singlet only transforming under the Peccei-Quinn symmetry, which generates the ALP. Its couplings with fermions can continuously span over many orders of magnitude, which constitutes a specific feature of this model in contr"},"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":"2402.14059","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-21T19:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"a2b5f766482c3ae695d2ec40c6164ce288a8aa9b39922c6a87de1a038a12ed30","abstract_canon_sha256":"3420cd38b4f058139e481adefe036720b337cfba7cd2d09a66c970da991a570c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:11:07.820730Z","signature_b64":"3QRE9bQ7V9BuqRGj/TS+Qhyn+Bi6HhgwrHZbu7Q1McvYlIjoXZBkYCUkQwVpm2Uyi3/vOXhD6tU0X19ZaGIFBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"54e0b76e9b6b4dd4a7da03af4d2c45ef2cb80a01ce3b5be58fd00e4587994058","last_reissued_at":"2026-07-05T10:11:07.820209Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:11:07.820209Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Visible GeV ALP from TeV Vector-like Leptons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arturo de Giorgi, Luca Merlo, Marta Fuentes Zamoro","submitted_at":"2024-02-21T19:00:01Z","abstract_excerpt":"We present a model where a GeV axion-like-particle (ALP) is predicted in a large portion of the parameter space due to the presence of explicit Peccei-Quinn symmetry-breaking terms in an exotic leptonic sector. The latter provides a solution to the muon $g-2$ anomaly, within the framework of the Linear Seesaw neutrino mechanism. The spectrum is extended by a complex scalar singlet only transforming under the Peccei-Quinn symmetry, which generates the ALP. Its couplings with fermions can continuously span over many orders of magnitude, which constitutes a specific feature of this model in contr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.14059","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2402.14059/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":"2402.14059","created_at":"2026-07-05T10:11:07.820279+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.14059v2","created_at":"2026-07-05T10:11:07.820279+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.14059","created_at":"2026-07-05T10:11:07.820279+00:00"},{"alias_kind":"pith_short_12","alias_value":"KTQLO3U3NNG5","created_at":"2026-07-05T10:11:07.820279+00:00"},{"alias_kind":"pith_short_16","alias_value":"KTQLO3U3NNG5JJ62","created_at":"2026-07-05T10:11:07.820279+00:00"},{"alias_kind":"pith_short_8","alias_value":"KTQLO3U3","created_at":"2026-07-05T10:11:07.820279+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.06787","citing_title":"The structure of multi-axion solutions to the strong CP problem","ref_index":133,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06787","citing_title":"The structure of multi-axion solutions to the strong CP problem","ref_index":129,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KTQLO3U3NNG5JJ62AOXU2LCF54","json":"https://pith.science/pith/KTQLO3U3NNG5JJ62AOXU2LCF54.json","graph_json":"https://pith.science/api/pith-number/KTQLO3U3NNG5JJ62AOXU2LCF54/graph.json","events_json":"https://pith.science/api/pith-number/KTQLO3U3NNG5JJ62AOXU2LCF54/events.json","paper":"https://pith.science/paper/KTQLO3U3"},"agent_actions":{"view_html":"https://pith.science/pith/KTQLO3U3NNG5JJ62AOXU2LCF54","download_json":"https://pith.science/pith/KTQLO3U3NNG5JJ62AOXU2LCF54.json","view_paper":"https://pith.science/paper/KTQLO3U3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.14059&json=true","fetch_graph":"https://pith.science/api/pith-number/KTQLO3U3NNG5JJ62AOXU2LCF54/graph.json","fetch_events":"https://pith.science/api/pith-number/KTQLO3U3NNG5JJ62AOXU2LCF54/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KTQLO3U3NNG5JJ62AOXU2LCF54/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KTQLO3U3NNG5JJ62AOXU2LCF54/action/storage_attestation","attest_author":"https://pith.science/pith/KTQLO3U3NNG5JJ62AOXU2LCF54/action/author_attestation","sign_citation":"https://pith.science/pith/KTQLO3U3NNG5JJ62AOXU2LCF54/action/citation_signature","submit_replication":"https://pith.science/pith/KTQLO3U3NNG5JJ62AOXU2LCF54/action/replication_record"}},"created_at":"2026-07-05T10:11:07.820279+00:00","updated_at":"2026-07-05T10:11:07.820279+00:00"}