{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:N5ALIJDQGZ75ILMP6NQRH5PXVB","short_pith_number":"pith:N5ALIJDQ","schema_version":"1.0","canonical_sha256":"6f40b42470367fd42d8ff36113f5f7a8751ea055b8d3931a6dc3e6ca600ece62","source":{"kind":"arxiv","id":"1206.6140","version":3},"attestation_state":"computed","paper":{"title":"Large, negative threshold contributions to light soft masses in models with Effective Supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Tamarit","submitted_at":"2012-06-26T23:25:30Z","abstract_excerpt":"Threshold contributions to light scalar soft masses due to heavy sparticles (possibly including a heavy Higgs mostly aligned with H_d) in Effective SUSY scenarios are dominated by two-loop diagrams involving gauge couplings. This is due to the fact that in the limit in which the heavy states are degenerate, their one-loop contributions to the light soft masses only depend on small Yukawas and the hypercharge coupling. The two-loop threshold corrections involving only gauge couplings are calculated accounting for nonzero gaugino and light squark masses and shown to be negative, and rather large"},"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":"1206.6140","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-06-26T23:25:30Z","cross_cats_sorted":[],"title_canon_sha256":"06cf5cc843eca81c32089e44d0c68aab86bf49e7d90722740b29c9143db63f3f","abstract_canon_sha256":"caeeafb6ccd83ff1768c26d8617d006a62f3bfb886bf36a3f679f7f372e44ebb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:39:16.377249Z","signature_b64":"ogkkc9KyNLC22r5jAcS2nqeLUOA4aMlubxUdpkyfWC7vhinWLO2uTeQ5VX4FId3qEd5DjtIsAL1HUnXsu3ctAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6f40b42470367fd42d8ff36113f5f7a8751ea055b8d3931a6dc3e6ca600ece62","last_reissued_at":"2026-05-18T03:39:16.376667Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:39:16.376667Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large, negative threshold contributions to light soft masses in models with Effective Supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Tamarit","submitted_at":"2012-06-26T23:25:30Z","abstract_excerpt":"Threshold contributions to light scalar soft masses due to heavy sparticles (possibly including a heavy Higgs mostly aligned with H_d) in Effective SUSY scenarios are dominated by two-loop diagrams involving gauge couplings. This is due to the fact that in the limit in which the heavy states are degenerate, their one-loop contributions to the light soft masses only depend on small Yukawas and the hypercharge coupling. The two-loop threshold corrections involving only gauge couplings are calculated accounting for nonzero gaugino and light squark masses and shown to be negative, and rather large"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.6140","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":"1206.6140","created_at":"2026-05-18T03:39:16.376774+00:00"},{"alias_kind":"arxiv_version","alias_value":"1206.6140v3","created_at":"2026-05-18T03:39:16.376774+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.6140","created_at":"2026-05-18T03:39:16.376774+00:00"},{"alias_kind":"pith_short_12","alias_value":"N5ALIJDQGZ75","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_16","alias_value":"N5ALIJDQGZ75ILMP","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_8","alias_value":"N5ALIJDQ","created_at":"2026-05-18T12:27:16.716162+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/N5ALIJDQGZ75ILMP6NQRH5PXVB","json":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB.json","graph_json":"https://pith.science/api/pith-number/N5ALIJDQGZ75ILMP6NQRH5PXVB/graph.json","events_json":"https://pith.science/api/pith-number/N5ALIJDQGZ75ILMP6NQRH5PXVB/events.json","paper":"https://pith.science/paper/N5ALIJDQ"},"agent_actions":{"view_html":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB","download_json":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB.json","view_paper":"https://pith.science/paper/N5ALIJDQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1206.6140&json=true","fetch_graph":"https://pith.science/api/pith-number/N5ALIJDQGZ75ILMP6NQRH5PXVB/graph.json","fetch_events":"https://pith.science/api/pith-number/N5ALIJDQGZ75ILMP6NQRH5PXVB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/action/storage_attestation","attest_author":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/action/author_attestation","sign_citation":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/action/citation_signature","submit_replication":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/action/replication_record"}},"created_at":"2026-05-18T03:39:16.376774+00:00","updated_at":"2026-05-18T03:39:16.376774+00:00"}