{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:IIX7SC7NKDOYO6VJLFY2ZVCOG5","short_pith_number":"pith:IIX7SC7N","schema_version":"1.0","canonical_sha256":"422ff90bed50dd877aa95971acd44e375be42cde1376bc4d52c92ff00be68f45","source":{"kind":"arxiv","id":"hep-th/9804068","version":1},"attestation_state":"computed","paper":{"title":"Exact results for non-holomorphic masses in softly broken supersymmetric gauge theories","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Nima Arkani-Hamed, Riccardo Rattazzi","submitted_at":"1998-04-08T23:42:10Z","abstract_excerpt":"We consider strongly coupled supersymmetric gauge theories softly broken by the addition of gaugino masses $m_\\lambda$ and (non-holomorphic) scalar masses $m^2$, taken to be small relative to the dynamical scale $\\Lambda$. For theories with a weakly coupled dual description in the infrared, we compute exactly the leading soft masses for the \"magnetic\" degrees of freedom, with uncalculable corrections suppressed by powers of $(m_{\\lambda}/\\Lambda), (m/\\Lambda)$. The exact relations hold between the infrared fixed point \"magnetic\" soft masses and the ultraviolet fixed point \"electric\" soft masse"},"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":"hep-th/9804068","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-04-08T23:42:10Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"bd6adaecf2c07182b78ab613a580b91a516ca630e257c1b43497dc19bcbe2ebb","abstract_canon_sha256":"351236a4c7c192d9920e76b2e53fccde9745e803916c9aa8e29ac15d909b4f0a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:09:45.732353Z","signature_b64":"Sjbs/iPzEWxSdyT35X/nSvHtUthATayJ7RqCxbOBcip4DdKD0f9MQF/AGBzEJvCr3bhsUMHuDZoOfLDxxzI3AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"422ff90bed50dd877aa95971acd44e375be42cde1376bc4d52c92ff00be68f45","last_reissued_at":"2026-07-04T16:09:45.732003Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:09:45.732003Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exact results for non-holomorphic masses in softly broken supersymmetric gauge theories","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Nima Arkani-Hamed, Riccardo Rattazzi","submitted_at":"1998-04-08T23:42:10Z","abstract_excerpt":"We consider strongly coupled supersymmetric gauge theories softly broken by the addition of gaugino masses $m_\\lambda$ and (non-holomorphic) scalar masses $m^2$, taken to be small relative to the dynamical scale $\\Lambda$. For theories with a weakly coupled dual description in the infrared, we compute exactly the leading soft masses for the \"magnetic\" degrees of freedom, with uncalculable corrections suppressed by powers of $(m_{\\lambda}/\\Lambda), (m/\\Lambda)$. The exact relations hold between the infrared fixed point \"magnetic\" soft masses and the ultraviolet fixed point \"electric\" soft masse"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9804068","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/hep-th/9804068/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":"hep-th/9804068","created_at":"2026-07-04T16:09:45.732062+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9804068v1","created_at":"2026-07-04T16:09:45.732062+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9804068","created_at":"2026-07-04T16:09:45.732062+00:00"},{"alias_kind":"pith_short_12","alias_value":"IIX7SC7NKDOY","created_at":"2026-07-04T16:09:45.732062+00:00"},{"alias_kind":"pith_short_16","alias_value":"IIX7SC7NKDOYO6VJ","created_at":"2026-07-04T16:09:45.732062+00:00"},{"alias_kind":"pith_short_8","alias_value":"IIX7SC7N","created_at":"2026-07-04T16:09:45.732062+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/IIX7SC7NKDOYO6VJLFY2ZVCOG5","json":"https://pith.science/pith/IIX7SC7NKDOYO6VJLFY2ZVCOG5.json","graph_json":"https://pith.science/api/pith-number/IIX7SC7NKDOYO6VJLFY2ZVCOG5/graph.json","events_json":"https://pith.science/api/pith-number/IIX7SC7NKDOYO6VJLFY2ZVCOG5/events.json","paper":"https://pith.science/paper/IIX7SC7N"},"agent_actions":{"view_html":"https://pith.science/pith/IIX7SC7NKDOYO6VJLFY2ZVCOG5","download_json":"https://pith.science/pith/IIX7SC7NKDOYO6VJLFY2ZVCOG5.json","view_paper":"https://pith.science/paper/IIX7SC7N","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9804068&json=true","fetch_graph":"https://pith.science/api/pith-number/IIX7SC7NKDOYO6VJLFY2ZVCOG5/graph.json","fetch_events":"https://pith.science/api/pith-number/IIX7SC7NKDOYO6VJLFY2ZVCOG5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IIX7SC7NKDOYO6VJLFY2ZVCOG5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IIX7SC7NKDOYO6VJLFY2ZVCOG5/action/storage_attestation","attest_author":"https://pith.science/pith/IIX7SC7NKDOYO6VJLFY2ZVCOG5/action/author_attestation","sign_citation":"https://pith.science/pith/IIX7SC7NKDOYO6VJLFY2ZVCOG5/action/citation_signature","submit_replication":"https://pith.science/pith/IIX7SC7NKDOYO6VJLFY2ZVCOG5/action/replication_record"}},"created_at":"2026-07-04T16:09:45.732062+00:00","updated_at":"2026-07-04T16:09:45.732062+00:00"}