{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:B7GIUGJEPE547QJZZUNBQ74KXN","short_pith_number":"pith:B7GIUGJE","schema_version":"1.0","canonical_sha256":"0fcc8a1924793bcfc139cd1a187f8abb4b8b7bfffb3accae4a1c983abffbf2c4","source":{"kind":"arxiv","id":"1104.1573","version":3},"attestation_state":"computed","paper":{"title":"SPheno 3.1: extensions including flavour, CP-phases and models beyond the MSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"F. Staub, W. Porod","submitted_at":"2011-04-08T13:48:02Z","abstract_excerpt":"We describe recent extensions of the program SPheno including flavour aspects, CP-phases, R-parity violation and low energy observables. In case of flavour mixing all masses of supersymmetric particles are calculated including the complete flavour structure and all possible CP-phases at the 1-loop level. We give details on implemented seesaw models, low energy observables and the corresponding extension of the SUSY Les Houches Accord. Moreover, we comment on the possiblities to include MSSM extensions in SPheno."},"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":"1104.1573","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-04-08T13:48:02Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"e4a180186a04d32177b1ed5d265e72cff7dec1911a1ea92a8329ca269553ac96","abstract_canon_sha256":"7ccd7d48e96c3587347fddfb87c473215da4696ee6428928667fe966ce055ef5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:50:35.675617Z","signature_b64":"jFLezIu1EDJxHRbXRlMWvbJF3+Y3y0L7tYF4MTULmFh1m6X4ZjGwe3g2sR3isUqmVHxxUqepadaEwXZOk03lCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0fcc8a1924793bcfc139cd1a187f8abb4b8b7bfffb3accae4a1c983abffbf2c4","last_reissued_at":"2026-05-18T03:50:35.675032Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:50:35.675032Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SPheno 3.1: extensions including flavour, CP-phases and models beyond the MSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"F. Staub, W. Porod","submitted_at":"2011-04-08T13:48:02Z","abstract_excerpt":"We describe recent extensions of the program SPheno including flavour aspects, CP-phases, R-parity violation and low energy observables. In case of flavour mixing all masses of supersymmetric particles are calculated including the complete flavour structure and all possible CP-phases at the 1-loop level. We give details on implemented seesaw models, low energy observables and the corresponding extension of the SUSY Les Houches Accord. Moreover, we comment on the possiblities to include MSSM extensions in SPheno."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.1573","kind":"arxiv","version":3},"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":"1104.1573","created_at":"2026-05-18T03:50:35.675127+00:00"},{"alias_kind":"arxiv_version","alias_value":"1104.1573v3","created_at":"2026-05-18T03:50:35.675127+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.1573","created_at":"2026-05-18T03:50:35.675127+00:00"},{"alias_kind":"pith_short_12","alias_value":"B7GIUGJEPE54","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_16","alias_value":"B7GIUGJEPE547QJZ","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_8","alias_value":"B7GIUGJE","created_at":"2026-05-18T12:26:24.575870+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2507.08927","citing_title":"Deciphering compressed electroweakino excesses with MadAnalysis 5","ref_index":96,"is_internal_anchor":true},{"citing_arxiv_id":"2605.15286","citing_title":"Predicting Three Generations of Fermions: Discovery Prospects of the Bilepton Model","ref_index":23,"is_internal_anchor":true},{"citing_arxiv_id":"2506.04370","citing_title":"Dark Matter Induced Proton Decays","ref_index":73,"is_internal_anchor":true},{"citing_arxiv_id":"2605.05312","citing_title":"Monochromatic neutrinos from scotogenic dark matter","ref_index":42,"is_internal_anchor":true},{"citing_arxiv_id":"2605.00098","citing_title":"The neutral scalars of type-II 2HDM+S under the LHC","ref_index":23,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B7GIUGJEPE547QJZZUNBQ74KXN","json":"https://pith.science/pith/B7GIUGJEPE547QJZZUNBQ74KXN.json","graph_json":"https://pith.science/api/pith-number/B7GIUGJEPE547QJZZUNBQ74KXN/graph.json","events_json":"https://pith.science/api/pith-number/B7GIUGJEPE547QJZZUNBQ74KXN/events.json","paper":"https://pith.science/paper/B7GIUGJE"},"agent_actions":{"view_html":"https://pith.science/pith/B7GIUGJEPE547QJZZUNBQ74KXN","download_json":"https://pith.science/pith/B7GIUGJEPE547QJZZUNBQ74KXN.json","view_paper":"https://pith.science/paper/B7GIUGJE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1104.1573&json=true","fetch_graph":"https://pith.science/api/pith-number/B7GIUGJEPE547QJZZUNBQ74KXN/graph.json","fetch_events":"https://pith.science/api/pith-number/B7GIUGJEPE547QJZZUNBQ74KXN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B7GIUGJEPE547QJZZUNBQ74KXN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B7GIUGJEPE547QJZZUNBQ74KXN/action/storage_attestation","attest_author":"https://pith.science/pith/B7GIUGJEPE547QJZZUNBQ74KXN/action/author_attestation","sign_citation":"https://pith.science/pith/B7GIUGJEPE547QJZZUNBQ74KXN/action/citation_signature","submit_replication":"https://pith.science/pith/B7GIUGJEPE547QJZZUNBQ74KXN/action/replication_record"}},"created_at":"2026-05-18T03:50:35.675127+00:00","updated_at":"2026-05-18T03:50:35.675127+00:00"}