{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:UDSPUMWQQWXAVQXUCJ3KRIVDS6","short_pith_number":"pith:UDSPUMWQ","schema_version":"1.0","canonical_sha256":"a0e4fa32d085ae0ac2f41276a8a2a3978bf3725fdf28e438eb48b84d5324bf56","source":{"kind":"arxiv","id":"2402.16491","version":2},"attestation_state":"computed","paper":{"title":"On Lepton Flavor Violation and Dark Matter in Scotogenic model with Trimaximal Mixing","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Sanjeev Kumar, Surender Verma, Tapender","submitted_at":"2024-02-26T11:16:25Z","abstract_excerpt":"We examine the Scotogenic model employing the TM$_2$ mixing matrix, $U_{\\text{TM}_2}$, for neutrinos and parameterize the Yukawa coupling matrix $y$ based on the diagonalization condition for the neutrino mass matrix, $m_{\\nu}$. Our investigation centers on analyzing the relic density of cold dark matter ($\\Omega h^2$) and possible lepton flavor violation (LFV) in the model. In particular, we study coannihilation dynamics and LFV, in the model, considering various coannihilation scenarios including non-zero mass splitting between lightest sterile neutrinos. While analyzing, we have taken into "},"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":"2402.16491","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-26T11:16:25Z","cross_cats_sorted":[],"title_canon_sha256":"23727c7c6014414cc61dc14d994d879f79b071632965b1335af9e42a6a7215f9","abstract_canon_sha256":"af224cb15c3b13d411fc9b3fe04f0c2339b8a7dd1b80ec8eca3b2b6a70add2be"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:36:46.054440Z","signature_b64":"IRmitfp1f7+eKqPexFffpwFe73IGc2F0qL5dF3VO2ISZOosFUzhYpWmmNBCMg39T7AJT+/Lcs0M4wRjik0A+BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0e4fa32d085ae0ac2f41276a8a2a3978bf3725fdf28e438eb48b84d5324bf56","last_reissued_at":"2026-07-05T08:36:46.053910Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:36:46.053910Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On Lepton Flavor Violation and Dark Matter in Scotogenic model with Trimaximal Mixing","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Sanjeev Kumar, Surender Verma, Tapender","submitted_at":"2024-02-26T11:16:25Z","abstract_excerpt":"We examine the Scotogenic model employing the TM$_2$ mixing matrix, $U_{\\text{TM}_2}$, for neutrinos and parameterize the Yukawa coupling matrix $y$ based on the diagonalization condition for the neutrino mass matrix, $m_{\\nu}$. Our investigation centers on analyzing the relic density of cold dark matter ($\\Omega h^2$) and possible lepton flavor violation (LFV) in the model. In particular, we study coannihilation dynamics and LFV, in the model, considering various coannihilation scenarios including non-zero mass splitting between lightest sterile neutrinos. While analyzing, we have taken into "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.16491","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/2402.16491/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":"2402.16491","created_at":"2026-07-05T08:36:46.053965+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.16491v2","created_at":"2026-07-05T08:36:46.053965+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.16491","created_at":"2026-07-05T08:36:46.053965+00:00"},{"alias_kind":"pith_short_12","alias_value":"UDSPUMWQQWXA","created_at":"2026-07-05T08:36:46.053965+00:00"},{"alias_kind":"pith_short_16","alias_value":"UDSPUMWQQWXAVQXU","created_at":"2026-07-05T08:36:46.053965+00:00"},{"alias_kind":"pith_short_8","alias_value":"UDSPUMWQ","created_at":"2026-07-05T08:36:46.053965+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.04733","citing_title":"Lepton flavor violation in the Majorana and Dirac scotogenic models","ref_index":88,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UDSPUMWQQWXAVQXUCJ3KRIVDS6","json":"https://pith.science/pith/UDSPUMWQQWXAVQXUCJ3KRIVDS6.json","graph_json":"https://pith.science/api/pith-number/UDSPUMWQQWXAVQXUCJ3KRIVDS6/graph.json","events_json":"https://pith.science/api/pith-number/UDSPUMWQQWXAVQXUCJ3KRIVDS6/events.json","paper":"https://pith.science/paper/UDSPUMWQ"},"agent_actions":{"view_html":"https://pith.science/pith/UDSPUMWQQWXAVQXUCJ3KRIVDS6","download_json":"https://pith.science/pith/UDSPUMWQQWXAVQXUCJ3KRIVDS6.json","view_paper":"https://pith.science/paper/UDSPUMWQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.16491&json=true","fetch_graph":"https://pith.science/api/pith-number/UDSPUMWQQWXAVQXUCJ3KRIVDS6/graph.json","fetch_events":"https://pith.science/api/pith-number/UDSPUMWQQWXAVQXUCJ3KRIVDS6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UDSPUMWQQWXAVQXUCJ3KRIVDS6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UDSPUMWQQWXAVQXUCJ3KRIVDS6/action/storage_attestation","attest_author":"https://pith.science/pith/UDSPUMWQQWXAVQXUCJ3KRIVDS6/action/author_attestation","sign_citation":"https://pith.science/pith/UDSPUMWQQWXAVQXUCJ3KRIVDS6/action/citation_signature","submit_replication":"https://pith.science/pith/UDSPUMWQQWXAVQXUCJ3KRIVDS6/action/replication_record"}},"created_at":"2026-07-05T08:36:46.053965+00:00","updated_at":"2026-07-05T08:36:46.053965+00:00"}