{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:PIBGVXVKKBL5X6KVII424WNTIS","short_pith_number":"pith:PIBGVXVK","schema_version":"1.0","canonical_sha256":"7a026adeaa5057dbf9554239ae59b3448737efc782f270d407e9019cf093e4a1","source":{"kind":"arxiv","id":"2012.11623","version":1},"attestation_state":"computed","paper":{"title":"Nucleon decay in the R-parity violating MSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Florian Domingo, Herbert K. Dreiner, Nidal Chamoun","submitted_at":"2020-12-21T19:00:13Z","abstract_excerpt":"We present a reanalysis of nucleon decay in the context of the R-parity violating MSSM, updating bounds on R-parity violating parameters against recent experimental and lattice results. We pay particular attention to the derivation of these constraints and specifically to the hadronic matrix elements, which usually stand as the limiting factor in order to derive reliable bounds, except for these few channels that have been studied on the lattice."},"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":"2012.11623","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-12-21T19:00:13Z","cross_cats_sorted":[],"title_canon_sha256":"9ee94a9f8ad40878e9dbe62c7af4de764c1b5c8c35fe991e173258a415430d81","abstract_canon_sha256":"69b07fd7ec37875d34b298ec0c1d66a3cf1fde070ba5c627aa5fbe1a8a26407f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:01:12.513620Z","signature_b64":"5NMDayXjnyHx1euCPj9fXRexCJQHPwA0w8MjTnR4fZnAE9hL94LTU3gSxXXPNpHn0flvasnApPtkAGLP/6e2CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7a026adeaa5057dbf9554239ae59b3448737efc782f270d407e9019cf093e4a1","last_reissued_at":"2026-07-05T03:01:12.513103Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:01:12.513103Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nucleon decay in the R-parity violating MSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Florian Domingo, Herbert K. Dreiner, Nidal Chamoun","submitted_at":"2020-12-21T19:00:13Z","abstract_excerpt":"We present a reanalysis of nucleon decay in the context of the R-parity violating MSSM, updating bounds on R-parity violating parameters against recent experimental and lattice results. We pay particular attention to the derivation of these constraints and specifically to the hadronic matrix elements, which usually stand as the limiting factor in order to derive reliable bounds, except for these few channels that have been studied on the lattice."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.11623","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2012.11623/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":"2012.11623","created_at":"2026-07-05T03:01:12.513173+00:00"},{"alias_kind":"arxiv_version","alias_value":"2012.11623v1","created_at":"2026-07-05T03:01:12.513173+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.11623","created_at":"2026-07-05T03:01:12.513173+00:00"},{"alias_kind":"pith_short_12","alias_value":"PIBGVXVKKBL5","created_at":"2026-07-05T03:01:12.513173+00:00"},{"alias_kind":"pith_short_16","alias_value":"PIBGVXVKKBL5X6KV","created_at":"2026-07-05T03:01:12.513173+00:00"},{"alias_kind":"pith_short_8","alias_value":"PIBGVXVK","created_at":"2026-07-05T03:01:12.513173+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.00830","citing_title":"$n \\to K\\ell$ and the baryon asymmetry of the universe","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21065","citing_title":"The Single Photon Signature of a Light Long-lived Neutralino at Remote Detectors at the LHC","ref_index":63,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PIBGVXVKKBL5X6KVII424WNTIS","json":"https://pith.science/pith/PIBGVXVKKBL5X6KVII424WNTIS.json","graph_json":"https://pith.science/api/pith-number/PIBGVXVKKBL5X6KVII424WNTIS/graph.json","events_json":"https://pith.science/api/pith-number/PIBGVXVKKBL5X6KVII424WNTIS/events.json","paper":"https://pith.science/paper/PIBGVXVK"},"agent_actions":{"view_html":"https://pith.science/pith/PIBGVXVKKBL5X6KVII424WNTIS","download_json":"https://pith.science/pith/PIBGVXVKKBL5X6KVII424WNTIS.json","view_paper":"https://pith.science/paper/PIBGVXVK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2012.11623&json=true","fetch_graph":"https://pith.science/api/pith-number/PIBGVXVKKBL5X6KVII424WNTIS/graph.json","fetch_events":"https://pith.science/api/pith-number/PIBGVXVKKBL5X6KVII424WNTIS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PIBGVXVKKBL5X6KVII424WNTIS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PIBGVXVKKBL5X6KVII424WNTIS/action/storage_attestation","attest_author":"https://pith.science/pith/PIBGVXVKKBL5X6KVII424WNTIS/action/author_attestation","sign_citation":"https://pith.science/pith/PIBGVXVKKBL5X6KVII424WNTIS/action/citation_signature","submit_replication":"https://pith.science/pith/PIBGVXVKKBL5X6KVII424WNTIS/action/replication_record"}},"created_at":"2026-07-05T03:01:12.513173+00:00","updated_at":"2026-07-05T03:01:12.513173+00:00"}