{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:GRAH4YWQ55WN6VW262LD4LUMOQ","short_pith_number":"pith:GRAH4YWQ","schema_version":"1.0","canonical_sha256":"34407e62d0ef6cdf56daf6963e2e8c740e81a29296f61b91b81541e52674a42f","source":{"kind":"arxiv","id":"1302.6266","version":1},"attestation_state":"computed","paper":{"title":"Radiative Scaling Neutrino Mass with $A_4$ Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ahmed Rashed, Alexander Natale, Ernest Ma, Subhaditya Bhattacharya","submitted_at":"2013-02-25T22:23:45Z","abstract_excerpt":"A new idea for neutrino mass was proposed recently, where its smallness is not due to the seesaw mechanism, i.e. not inversely proportional to some large mass scale. It comes from a one-loop mechanism with dark matter in the loop consisting of singlet Majorana fermions $N_i$ with masses of order 10 keV and neutrino masses are scaled down from them by factors of about $10^{-5}$. We discuss how this model may be implemented with the non-Abelian discrete symmetry $A_4$ for neutrino mixing, and consider the phenomenology of $N_i$ as well as the extra scalar doublet $(\\eta^+,\\eta^0)$."},"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":"1302.6266","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-25T22:23:45Z","cross_cats_sorted":[],"title_canon_sha256":"ae8a92f048dd55563b06a5484ed8222023721c7b179825014b40943ba5f2bcfd","abstract_canon_sha256":"bca52bd7c0fa8404986d02d3ccf1497e99c4088e40237418ff635d213771c146"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:21:45.231285Z","signature_b64":"ACWU2cNLN2LqVInxxY5cg6CyzONwiwqqHz0YoDK5KfVcvjoFyt19JjKsnZ3rZ0BnatEJavh7mG/qAfDDdr7iCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"34407e62d0ef6cdf56daf6963e2e8c740e81a29296f61b91b81541e52674a42f","last_reissued_at":"2026-05-18T03:21:45.230397Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:21:45.230397Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Radiative Scaling Neutrino Mass with $A_4$ Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ahmed Rashed, Alexander Natale, Ernest Ma, Subhaditya Bhattacharya","submitted_at":"2013-02-25T22:23:45Z","abstract_excerpt":"A new idea for neutrino mass was proposed recently, where its smallness is not due to the seesaw mechanism, i.e. not inversely proportional to some large mass scale. It comes from a one-loop mechanism with dark matter in the loop consisting of singlet Majorana fermions $N_i$ with masses of order 10 keV and neutrino masses are scaled down from them by factors of about $10^{-5}$. We discuss how this model may be implemented with the non-Abelian discrete symmetry $A_4$ for neutrino mixing, and consider the phenomenology of $N_i$ as well as the extra scalar doublet $(\\eta^+,\\eta^0)$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.6266","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":"1302.6266","created_at":"2026-05-18T03:21:45.230551+00:00"},{"alias_kind":"arxiv_version","alias_value":"1302.6266v1","created_at":"2026-05-18T03:21:45.230551+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.6266","created_at":"2026-05-18T03:21:45.230551+00:00"},{"alias_kind":"pith_short_12","alias_value":"GRAH4YWQ55WN","created_at":"2026-05-18T12:27:45.050594+00:00"},{"alias_kind":"pith_short_16","alias_value":"GRAH4YWQ55WN6VW2","created_at":"2026-05-18T12:27:45.050594+00:00"},{"alias_kind":"pith_short_8","alias_value":"GRAH4YWQ","created_at":"2026-05-18T12:27:45.050594+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/GRAH4YWQ55WN6VW262LD4LUMOQ","json":"https://pith.science/pith/GRAH4YWQ55WN6VW262LD4LUMOQ.json","graph_json":"https://pith.science/api/pith-number/GRAH4YWQ55WN6VW262LD4LUMOQ/graph.json","events_json":"https://pith.science/api/pith-number/GRAH4YWQ55WN6VW262LD4LUMOQ/events.json","paper":"https://pith.science/paper/GRAH4YWQ"},"agent_actions":{"view_html":"https://pith.science/pith/GRAH4YWQ55WN6VW262LD4LUMOQ","download_json":"https://pith.science/pith/GRAH4YWQ55WN6VW262LD4LUMOQ.json","view_paper":"https://pith.science/paper/GRAH4YWQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1302.6266&json=true","fetch_graph":"https://pith.science/api/pith-number/GRAH4YWQ55WN6VW262LD4LUMOQ/graph.json","fetch_events":"https://pith.science/api/pith-number/GRAH4YWQ55WN6VW262LD4LUMOQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GRAH4YWQ55WN6VW262LD4LUMOQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GRAH4YWQ55WN6VW262LD4LUMOQ/action/storage_attestation","attest_author":"https://pith.science/pith/GRAH4YWQ55WN6VW262LD4LUMOQ/action/author_attestation","sign_citation":"https://pith.science/pith/GRAH4YWQ55WN6VW262LD4LUMOQ/action/citation_signature","submit_replication":"https://pith.science/pith/GRAH4YWQ55WN6VW262LD4LUMOQ/action/replication_record"}},"created_at":"2026-05-18T03:21:45.230551+00:00","updated_at":"2026-05-18T03:21:45.230551+00:00"}