{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:SHJAW73Y4U5742T5AHOSUTOTGM","short_pith_number":"pith:SHJAW73Y","schema_version":"1.0","canonical_sha256":"91d20b7f78e53bfe6a7d01dd2a4dd33327a04404736117bdcebb531319e63204","source":{"kind":"arxiv","id":"1407.4081","version":2},"attestation_state":"computed","paper":{"title":"Higgs Mass and Unnatural Supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alessandro Strumia, Emanuele Bagnaschi, Gian F. Giudice, Pietro Slavich","submitted_at":"2014-07-15T18:13:43Z","abstract_excerpt":"Assuming that supersymmetry exists well above the weak scale, we derive the full one-loop matching conditions between the SM and the supersymmetric theory, allowing for the possibility of an intermediate Split-SUSY scale. We also compute two-loop QCD corrections to the matching condition of the Higgs quartic coupling. These results are used to improve the calculation of the Higgs mass in models with high-scale supersymmetry or split supersymmetry, reducing the theoretical uncertainty. We explore the phenomenology of a mini-split scenario with gaugino masses determined by anomaly mediation. Dep"},"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":"1407.4081","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-15T18:13:43Z","cross_cats_sorted":[],"title_canon_sha256":"8b7503ede896ba17dc1560ff38ef810c76e77d41ff15dc75dfa0561560d43c49","abstract_canon_sha256":"895009c63ab4661e3e0f7a2309bb75d6640f66ccf45c3aa13ae084e7f92cef8f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:42:38.972650Z","signature_b64":"JOM+2nEwcr4Iv6P3APEcW56PxPNxWJ8UV5ByGiDSCbEk4dygkly2FbvbPIw5XgBMPe0qRNmr4+Q99rFrABXICQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"91d20b7f78e53bfe6a7d01dd2a4dd33327a04404736117bdcebb531319e63204","last_reissued_at":"2026-05-18T02:42:38.972073Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:42:38.972073Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs Mass and Unnatural Supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alessandro Strumia, Emanuele Bagnaschi, Gian F. Giudice, Pietro Slavich","submitted_at":"2014-07-15T18:13:43Z","abstract_excerpt":"Assuming that supersymmetry exists well above the weak scale, we derive the full one-loop matching conditions between the SM and the supersymmetric theory, allowing for the possibility of an intermediate Split-SUSY scale. We also compute two-loop QCD corrections to the matching condition of the Higgs quartic coupling. These results are used to improve the calculation of the Higgs mass in models with high-scale supersymmetry or split supersymmetry, reducing the theoretical uncertainty. We explore the phenomenology of a mini-split scenario with gaugino masses determined by anomaly mediation. Dep"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.4081","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":"1407.4081","created_at":"2026-05-18T02:42:38.972166+00:00"},{"alias_kind":"arxiv_version","alias_value":"1407.4081v2","created_at":"2026-05-18T02:42:38.972166+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.4081","created_at":"2026-05-18T02:42:38.972166+00:00"},{"alias_kind":"pith_short_12","alias_value":"SHJAW73Y4U57","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"SHJAW73Y4U5742T5","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"SHJAW73Y","created_at":"2026-05-18T12:28:49.207871+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2506.05201","citing_title":"SUSY meets SMEFT: Complete one-loop matching of the general MSSM","ref_index":73,"is_internal_anchor":true},{"citing_arxiv_id":"2602.05623","citing_title":"Induced-Gravity Palatini-Like Higgs Inflation in Supergravity Confronts ACT DR6","ref_index":110,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SHJAW73Y4U5742T5AHOSUTOTGM","json":"https://pith.science/pith/SHJAW73Y4U5742T5AHOSUTOTGM.json","graph_json":"https://pith.science/api/pith-number/SHJAW73Y4U5742T5AHOSUTOTGM/graph.json","events_json":"https://pith.science/api/pith-number/SHJAW73Y4U5742T5AHOSUTOTGM/events.json","paper":"https://pith.science/paper/SHJAW73Y"},"agent_actions":{"view_html":"https://pith.science/pith/SHJAW73Y4U5742T5AHOSUTOTGM","download_json":"https://pith.science/pith/SHJAW73Y4U5742T5AHOSUTOTGM.json","view_paper":"https://pith.science/paper/SHJAW73Y","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1407.4081&json=true","fetch_graph":"https://pith.science/api/pith-number/SHJAW73Y4U5742T5AHOSUTOTGM/graph.json","fetch_events":"https://pith.science/api/pith-number/SHJAW73Y4U5742T5AHOSUTOTGM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SHJAW73Y4U5742T5AHOSUTOTGM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SHJAW73Y4U5742T5AHOSUTOTGM/action/storage_attestation","attest_author":"https://pith.science/pith/SHJAW73Y4U5742T5AHOSUTOTGM/action/author_attestation","sign_citation":"https://pith.science/pith/SHJAW73Y4U5742T5AHOSUTOTGM/action/citation_signature","submit_replication":"https://pith.science/pith/SHJAW73Y4U5742T5AHOSUTOTGM/action/replication_record"}},"created_at":"2026-05-18T02:42:38.972166+00:00","updated_at":"2026-05-18T02:42:38.972166+00:00"}