{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:JRSPCYM42VQA6FK7GO6SSF7XYJ","short_pith_number":"pith:JRSPCYM4","schema_version":"1.0","canonical_sha256":"4c64f1619cd5600f155f33bd2917f7c261894f39e01fd16204b47175ee487007","source":{"kind":"arxiv","id":"1601.07183","version":2},"attestation_state":"computed","paper":{"title":"N-Relaxion: Large Field Excursions from a Few Site Relaxion Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Camila S. Machado, Leonardo de Lima, Nayara Fonseca, Ricardo D. Matheus","submitted_at":"2016-01-26T21:00:08Z","abstract_excerpt":"Relaxion models are an interesting new avenue to explain the radiative stability of the Standard Model scalar sector. They require very large field excursions, which are difficult to generate in a consistent UV completion and to reconcile with the compact field space of the relaxion. We propose an N-site model which naturally generates the large decay constant needed to address these issues. Our model offers distinct advantages with respect to previous proposals: the construction involves non-abelian fields, allowing for controlled high energy behaviour and more model building possibilities, b"},"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":"1601.07183","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-01-26T21:00:08Z","cross_cats_sorted":[],"title_canon_sha256":"e4e3d4b3181d094537175750e3f91c4d15bd8ad2909ef94ed5f148b88ca22f2a","abstract_canon_sha256":"058aa7c6dec018add86d5779ba2413dc9237aecf074e18a565236f5f8b05e551"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:03:50.510774Z","signature_b64":"lzqdD1W6+AZ97k5BxsksxjuByUozy9J98kYHdE7CoqZB8Uj/oOvEIlNizq5gFVh+yevtGuF6SWTBb6ZngcUcDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4c64f1619cd5600f155f33bd2917f7c261894f39e01fd16204b47175ee487007","last_reissued_at":"2026-05-18T01:03:50.510114Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:03:50.510114Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"N-Relaxion: Large Field Excursions from a Few Site Relaxion Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Camila S. Machado, Leonardo de Lima, Nayara Fonseca, Ricardo D. Matheus","submitted_at":"2016-01-26T21:00:08Z","abstract_excerpt":"Relaxion models are an interesting new avenue to explain the radiative stability of the Standard Model scalar sector. They require very large field excursions, which are difficult to generate in a consistent UV completion and to reconcile with the compact field space of the relaxion. We propose an N-site model which naturally generates the large decay constant needed to address these issues. Our model offers distinct advantages with respect to previous proposals: the construction involves non-abelian fields, allowing for controlled high energy behaviour and more model building possibilities, b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.07183","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":"1601.07183","created_at":"2026-05-18T01:03:50.510212+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.07183v2","created_at":"2026-05-18T01:03:50.510212+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.07183","created_at":"2026-05-18T01:03:50.510212+00:00"},{"alias_kind":"pith_short_12","alias_value":"JRSPCYM42VQA","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_16","alias_value":"JRSPCYM42VQA6FK7","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_8","alias_value":"JRSPCYM4","created_at":"2026-05-18T12:30:25.849896+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/JRSPCYM42VQA6FK7GO6SSF7XYJ","json":"https://pith.science/pith/JRSPCYM42VQA6FK7GO6SSF7XYJ.json","graph_json":"https://pith.science/api/pith-number/JRSPCYM42VQA6FK7GO6SSF7XYJ/graph.json","events_json":"https://pith.science/api/pith-number/JRSPCYM42VQA6FK7GO6SSF7XYJ/events.json","paper":"https://pith.science/paper/JRSPCYM4"},"agent_actions":{"view_html":"https://pith.science/pith/JRSPCYM42VQA6FK7GO6SSF7XYJ","download_json":"https://pith.science/pith/JRSPCYM42VQA6FK7GO6SSF7XYJ.json","view_paper":"https://pith.science/paper/JRSPCYM4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.07183&json=true","fetch_graph":"https://pith.science/api/pith-number/JRSPCYM42VQA6FK7GO6SSF7XYJ/graph.json","fetch_events":"https://pith.science/api/pith-number/JRSPCYM42VQA6FK7GO6SSF7XYJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JRSPCYM42VQA6FK7GO6SSF7XYJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JRSPCYM42VQA6FK7GO6SSF7XYJ/action/storage_attestation","attest_author":"https://pith.science/pith/JRSPCYM42VQA6FK7GO6SSF7XYJ/action/author_attestation","sign_citation":"https://pith.science/pith/JRSPCYM42VQA6FK7GO6SSF7XYJ/action/citation_signature","submit_replication":"https://pith.science/pith/JRSPCYM42VQA6FK7GO6SSF7XYJ/action/replication_record"}},"created_at":"2026-05-18T01:03:50.510212+00:00","updated_at":"2026-05-18T01:03:50.510212+00:00"}