{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:2LQKR5RGPBU4B24K7LWSSQUFJY","short_pith_number":"pith:2LQKR5RG","schema_version":"1.0","canonical_sha256":"d2e0a8f6267869c0eb8afaed2942854e17110e3473e275688f67094141ea5b35","source":{"kind":"arxiv","id":"1710.05775","version":2},"attestation_state":"computed","paper":{"title":"Majorana Dark Matter in a new B-L model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Rukmani Mohanta, Shivaramakrishna Singirala, Soumya Rao, Sudhanwa Patra","submitted_at":"2017-10-16T15:13:50Z","abstract_excerpt":"We present a comprehensive study of Majorana dark matter in a $U(1)_{B-L}$ gauge extension of the standard model, where three exotic fermions with $B-L$ charges as $-4, -4, +5$ are added to make the model free from the triangle gauge anomalies. The enriched scalar sector and the new heavy gauge boson $Z^{\\prime},$ associated with the $U(1)_{B-L}$ symmetry make the model advantageous to be explored in dual portal scenarios for the search of dark matter signal. Diagonalizing the exotic fermion mass matrix, we obtain the Majorana mass eigenstates, of which the lightest one plays the role of dark "},"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":"1710.05775","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-16T15:13:50Z","cross_cats_sorted":[],"title_canon_sha256":"02b1eba5f9e7690cd0addbf08f4e4795e01797827e03e3fdc38af1034f28e219","abstract_canon_sha256":"2db6bc316fbd7e3a310973a86f171032f5d297e03b5dfa6567c352e7f746e5a3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:53.587929Z","signature_b64":"9Das8+wX5H/+980oRu5GyYIQ5Vus5rfg08wPBbOq/nnoUuDvs9YmayCu6Xbt/Zat2AP52DiEjTWVBFB+Y0D3AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d2e0a8f6267869c0eb8afaed2942854e17110e3473e275688f67094141ea5b35","last_reissued_at":"2026-05-17T23:59:53.587338Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:53.587338Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Majorana Dark Matter in a new B-L model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Rukmani Mohanta, Shivaramakrishna Singirala, Soumya Rao, Sudhanwa Patra","submitted_at":"2017-10-16T15:13:50Z","abstract_excerpt":"We present a comprehensive study of Majorana dark matter in a $U(1)_{B-L}$ gauge extension of the standard model, where three exotic fermions with $B-L$ charges as $-4, -4, +5$ are added to make the model free from the triangle gauge anomalies. The enriched scalar sector and the new heavy gauge boson $Z^{\\prime},$ associated with the $U(1)_{B-L}$ symmetry make the model advantageous to be explored in dual portal scenarios for the search of dark matter signal. Diagonalizing the exotic fermion mass matrix, we obtain the Majorana mass eigenstates, of which the lightest one plays the role of dark "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.05775","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":"1710.05775","created_at":"2026-05-17T23:59:53.587434+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.05775v2","created_at":"2026-05-17T23:59:53.587434+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.05775","created_at":"2026-05-17T23:59:53.587434+00:00"},{"alias_kind":"pith_short_12","alias_value":"2LQKR5RGPBU4","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_16","alias_value":"2LQKR5RGPBU4B24K","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_8","alias_value":"2LQKR5RG","created_at":"2026-05-18T12:30:55.937587+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/2LQKR5RGPBU4B24K7LWSSQUFJY","json":"https://pith.science/pith/2LQKR5RGPBU4B24K7LWSSQUFJY.json","graph_json":"https://pith.science/api/pith-number/2LQKR5RGPBU4B24K7LWSSQUFJY/graph.json","events_json":"https://pith.science/api/pith-number/2LQKR5RGPBU4B24K7LWSSQUFJY/events.json","paper":"https://pith.science/paper/2LQKR5RG"},"agent_actions":{"view_html":"https://pith.science/pith/2LQKR5RGPBU4B24K7LWSSQUFJY","download_json":"https://pith.science/pith/2LQKR5RGPBU4B24K7LWSSQUFJY.json","view_paper":"https://pith.science/paper/2LQKR5RG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.05775&json=true","fetch_graph":"https://pith.science/api/pith-number/2LQKR5RGPBU4B24K7LWSSQUFJY/graph.json","fetch_events":"https://pith.science/api/pith-number/2LQKR5RGPBU4B24K7LWSSQUFJY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2LQKR5RGPBU4B24K7LWSSQUFJY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2LQKR5RGPBU4B24K7LWSSQUFJY/action/storage_attestation","attest_author":"https://pith.science/pith/2LQKR5RGPBU4B24K7LWSSQUFJY/action/author_attestation","sign_citation":"https://pith.science/pith/2LQKR5RGPBU4B24K7LWSSQUFJY/action/citation_signature","submit_replication":"https://pith.science/pith/2LQKR5RGPBU4B24K7LWSSQUFJY/action/replication_record"}},"created_at":"2026-05-17T23:59:53.587434+00:00","updated_at":"2026-05-17T23:59:53.587434+00:00"}