{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:NAOYSRMBTQ63L56TJVE4KSW3IJ","short_pith_number":"pith:NAOYSRMB","schema_version":"1.0","canonical_sha256":"681d8945819c3db5f7d34d49c54adb425d05ec49654f4c45d07538a4cf54c612","source":{"kind":"arxiv","id":"1807.09769","version":1},"attestation_state":"computed","paper":{"title":"Axion mass prediction from minimal grand unification","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Andreas Ringwald, Carlos Tamarit, Luca Di Luzio","submitted_at":"2018-07-25T18:00:00Z","abstract_excerpt":"We propose a minimal realization of the Peccei Quinn mechanism in a realistic SU(5) model, where the axion mass is directly connected to the grand-unification scale. By taking into account constraints from proton decay, collider searches and gauge coupling unification, we predict the axion mass: $m_a \\in [4.8, 6.6]$ neV. The upper bound can be relaxed up to $m_a < 330$ neV, at the cost of tuning the flavour structure of the proton decay operators. The predicted mass window will be complementarily probed by the axion dark matter experiments ABRACADABRA and CASPER-Electric, which could provide a"},"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":"1807.09769","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2018-07-25T18:00:00Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"d6ecfb110c4bea6c45bbdb940b958356d6bea57fd8caee7f93fa94cd4ab6ec4a","abstract_canon_sha256":"3954de3670ec5b707a09692c8b34b22bdf629df06add88e18646cb31191e676b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:18.718167Z","signature_b64":"23zPeGK/96xs+/p9nNcQA1nKAdR/T9Q0jAMmrOZCnUfnNRngAXwiFM5rl/KpDLVQvcbAWY97hufCv+unVRsmDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"681d8945819c3db5f7d34d49c54adb425d05ec49654f4c45d07538a4cf54c612","last_reissued_at":"2026-05-18T00:00:18.717550Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:18.717550Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Axion mass prediction from minimal grand unification","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Andreas Ringwald, Carlos Tamarit, Luca Di Luzio","submitted_at":"2018-07-25T18:00:00Z","abstract_excerpt":"We propose a minimal realization of the Peccei Quinn mechanism in a realistic SU(5) model, where the axion mass is directly connected to the grand-unification scale. By taking into account constraints from proton decay, collider searches and gauge coupling unification, we predict the axion mass: $m_a \\in [4.8, 6.6]$ neV. The upper bound can be relaxed up to $m_a < 330$ neV, at the cost of tuning the flavour structure of the proton decay operators. The predicted mass window will be complementarily probed by the axion dark matter experiments ABRACADABRA and CASPER-Electric, which could provide a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.09769","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":""},"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":"1807.09769","created_at":"2026-05-18T00:00:18.717648+00:00"},{"alias_kind":"arxiv_version","alias_value":"1807.09769v1","created_at":"2026-05-18T00:00:18.717648+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.09769","created_at":"2026-05-18T00:00:18.717648+00:00"},{"alias_kind":"pith_short_12","alias_value":"NAOYSRMBTQ63","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_16","alias_value":"NAOYSRMBTQ63L56T","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_8","alias_value":"NAOYSRMB","created_at":"2026-05-18T12:32:40.477152+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":113,"is_internal_anchor":false},{"citing_arxiv_id":"2604.16602","citing_title":"DMRadio-Core: A new approach for GUT-scale axion searches","ref_index":19,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NAOYSRMBTQ63L56TJVE4KSW3IJ","json":"https://pith.science/pith/NAOYSRMBTQ63L56TJVE4KSW3IJ.json","graph_json":"https://pith.science/api/pith-number/NAOYSRMBTQ63L56TJVE4KSW3IJ/graph.json","events_json":"https://pith.science/api/pith-number/NAOYSRMBTQ63L56TJVE4KSW3IJ/events.json","paper":"https://pith.science/paper/NAOYSRMB"},"agent_actions":{"view_html":"https://pith.science/pith/NAOYSRMBTQ63L56TJVE4KSW3IJ","download_json":"https://pith.science/pith/NAOYSRMBTQ63L56TJVE4KSW3IJ.json","view_paper":"https://pith.science/paper/NAOYSRMB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1807.09769&json=true","fetch_graph":"https://pith.science/api/pith-number/NAOYSRMBTQ63L56TJVE4KSW3IJ/graph.json","fetch_events":"https://pith.science/api/pith-number/NAOYSRMBTQ63L56TJVE4KSW3IJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NAOYSRMBTQ63L56TJVE4KSW3IJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NAOYSRMBTQ63L56TJVE4KSW3IJ/action/storage_attestation","attest_author":"https://pith.science/pith/NAOYSRMBTQ63L56TJVE4KSW3IJ/action/author_attestation","sign_citation":"https://pith.science/pith/NAOYSRMBTQ63L56TJVE4KSW3IJ/action/citation_signature","submit_replication":"https://pith.science/pith/NAOYSRMBTQ63L56TJVE4KSW3IJ/action/replication_record"}},"created_at":"2026-05-18T00:00:18.717648+00:00","updated_at":"2026-05-18T00:00:18.717648+00:00"}