{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:W6OIPZNFH33O3P5I7BPQPU4PPH","short_pith_number":"pith:W6OIPZNF","schema_version":"1.0","canonical_sha256":"b79c87e5a53ef6edbfa8f85f07d38f79d0489788a2dee4ac50e9db7479bd6364","source":{"kind":"arxiv","id":"1109.2901","version":2},"attestation_state":"computed","paper":{"title":"R-parity Conservation via the Stueckelberg Mechanism: LHC and Dark Matter Signals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Daniel Feldman, Pavel Fileviez Perez, Pran Nath","submitted_at":"2011-09-13T20:00:08Z","abstract_excerpt":"We investigate the connection between the conservation of R-parity in supersymmetry and the Stueckelberg mechanism for the mass generation of the B-L vector gauge boson. It is shown that with universal boundary conditions for soft terms of sfermions in each family at the high scale and with the Stueckelberg mechanism for generating mass for the B-L gauge boson present in the theory, electric charge conservation guarantees the conservation of R-parity in the minimal B-L extended supersymmetric standard model. We also discuss non-minimal extensions. This includes extensions where the gauge symme"},"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":"1109.2901","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-09-13T20:00:08Z","cross_cats_sorted":[],"title_canon_sha256":"e2bfbafd1cc258ff32eea4963a19fb39f3d5d5488bf0b431eea2d302a80c6e1c","abstract_canon_sha256":"8c6612a7737bd2843b69d4c9a3c3c5e22b4f9f5f84c6441b78182fb15b378d12"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:03:42.920219Z","signature_b64":"0iuOOiZYjD2NqpkNONhGLnc+jJ7IzkbLNAnFA7wOpAoD79umyq1arHVFsuO5Mf6Ghu5RMcWiMru6TcL1ffx3BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b79c87e5a53ef6edbfa8f85f07d38f79d0489788a2dee4ac50e9db7479bd6364","last_reissued_at":"2026-05-18T04:03:42.919491Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:03:42.919491Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"R-parity Conservation via the Stueckelberg Mechanism: LHC and Dark Matter Signals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Daniel Feldman, Pavel Fileviez Perez, Pran Nath","submitted_at":"2011-09-13T20:00:08Z","abstract_excerpt":"We investigate the connection between the conservation of R-parity in supersymmetry and the Stueckelberg mechanism for the mass generation of the B-L vector gauge boson. It is shown that with universal boundary conditions for soft terms of sfermions in each family at the high scale and with the Stueckelberg mechanism for generating mass for the B-L gauge boson present in the theory, electric charge conservation guarantees the conservation of R-parity in the minimal B-L extended supersymmetric standard model. We also discuss non-minimal extensions. This includes extensions where the gauge symme"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.2901","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":"1109.2901","created_at":"2026-05-18T04:03:42.919588+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.2901v2","created_at":"2026-05-18T04:03:42.919588+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.2901","created_at":"2026-05-18T04:03:42.919588+00:00"},{"alias_kind":"pith_short_12","alias_value":"W6OIPZNFH33O","created_at":"2026-05-18T12:26:44.992195+00:00"},{"alias_kind":"pith_short_16","alias_value":"W6OIPZNFH33O3P5I","created_at":"2026-05-18T12:26:44.992195+00:00"},{"alias_kind":"pith_short_8","alias_value":"W6OIPZNF","created_at":"2026-05-18T12:26:44.992195+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.03286","citing_title":"Observing Dirac neutrinos in the cosmic microwave background","ref_index":39,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W6OIPZNFH33O3P5I7BPQPU4PPH","json":"https://pith.science/pith/W6OIPZNFH33O3P5I7BPQPU4PPH.json","graph_json":"https://pith.science/api/pith-number/W6OIPZNFH33O3P5I7BPQPU4PPH/graph.json","events_json":"https://pith.science/api/pith-number/W6OIPZNFH33O3P5I7BPQPU4PPH/events.json","paper":"https://pith.science/paper/W6OIPZNF"},"agent_actions":{"view_html":"https://pith.science/pith/W6OIPZNFH33O3P5I7BPQPU4PPH","download_json":"https://pith.science/pith/W6OIPZNFH33O3P5I7BPQPU4PPH.json","view_paper":"https://pith.science/paper/W6OIPZNF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.2901&json=true","fetch_graph":"https://pith.science/api/pith-number/W6OIPZNFH33O3P5I7BPQPU4PPH/graph.json","fetch_events":"https://pith.science/api/pith-number/W6OIPZNFH33O3P5I7BPQPU4PPH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W6OIPZNFH33O3P5I7BPQPU4PPH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W6OIPZNFH33O3P5I7BPQPU4PPH/action/storage_attestation","attest_author":"https://pith.science/pith/W6OIPZNFH33O3P5I7BPQPU4PPH/action/author_attestation","sign_citation":"https://pith.science/pith/W6OIPZNFH33O3P5I7BPQPU4PPH/action/citation_signature","submit_replication":"https://pith.science/pith/W6OIPZNFH33O3P5I7BPQPU4PPH/action/replication_record"}},"created_at":"2026-05-18T04:03:42.919588+00:00","updated_at":"2026-05-18T04:03:42.919588+00:00"}