{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:JFNSJ4OG66L2B5PKZVZ5A6RO3J","short_pith_number":"pith:JFNSJ4OG","schema_version":"1.0","canonical_sha256":"495b24f1c6f797a0f5eacd73d07a2eda7cca8113af702f73f030002e816e399b","source":{"kind":"arxiv","id":"hep-th/9612207","version":2},"attestation_state":"computed","paper":{"title":"Confinement in N=1 SUSY Gauge Theories and Model Building Tools","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Csaba Csaki (MIT), Martin Schmaltz (Boston U.), Witold Skiba (MIT)","submitted_at":"1996-12-19T18:47:44Z","abstract_excerpt":"We develop a systematic approach to confinement in N=1 supersymmetric theories. We identify simple necessary conditions for theories to confine without chiral symmetry breaking and to generate a superpotential non-perturbatively (s-confine). Applying these conditions we identify all N=1 theories with a single gauge group and no tree-level superpotential which s-confine. We give a complete list of the confined spectra and superpotentials. Some of these theories are of great interest for model building. We give several new examples of models which break supersymmetry dynamically."},"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/9612207","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-12-19T18:47:44Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"9fd77b37133e358a12668b595084ed08669fed9d165660885bd7b0f9bd8be44a","abstract_canon_sha256":"9a3c264240fd0debbfa3d2525458e7fa50eb72cf87880ffcc9c3cc48af0e6354"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:50:10.391971Z","signature_b64":"r0yA7mcF2a+pgptAjGj2KZHFc83q5dpJtFKt5JTrmQtqpEMt+kE0d4IDRzP6oYKacxD10wF8U0jTXiSIGMWYBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"495b24f1c6f797a0f5eacd73d07a2eda7cca8113af702f73f030002e816e399b","last_reissued_at":"2026-07-04T15:50:10.391593Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:50:10.391593Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Confinement in N=1 SUSY Gauge Theories and Model Building Tools","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Csaba Csaki (MIT), Martin Schmaltz (Boston U.), Witold Skiba (MIT)","submitted_at":"1996-12-19T18:47:44Z","abstract_excerpt":"We develop a systematic approach to confinement in N=1 supersymmetric theories. We identify simple necessary conditions for theories to confine without chiral symmetry breaking and to generate a superpotential non-perturbatively (s-confine). Applying these conditions we identify all N=1 theories with a single gauge group and no tree-level superpotential which s-confine. We give a complete list of the confined spectra and superpotentials. Some of these theories are of great interest for model building. We give several new examples of models which break supersymmetry dynamically."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9612207","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9612207/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/9612207","created_at":"2026-07-04T15:50:10.391656+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9612207v2","created_at":"2026-07-04T15:50:10.391656+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9612207","created_at":"2026-07-04T15:50:10.391656+00:00"},{"alias_kind":"pith_short_12","alias_value":"JFNSJ4OG66L2","created_at":"2026-07-04T15:50:10.391656+00:00"},{"alias_kind":"pith_short_16","alias_value":"JFNSJ4OG66L2B5PK","created_at":"2026-07-04T15:50:10.391656+00:00"},{"alias_kind":"pith_short_8","alias_value":"JFNSJ4OG","created_at":"2026-07-04T15:50:10.391656+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.28954","citing_title":"Heavy Axion from a Confining Mirror GUT","ref_index":38,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JFNSJ4OG66L2B5PKZVZ5A6RO3J","json":"https://pith.science/pith/JFNSJ4OG66L2B5PKZVZ5A6RO3J.json","graph_json":"https://pith.science/api/pith-number/JFNSJ4OG66L2B5PKZVZ5A6RO3J/graph.json","events_json":"https://pith.science/api/pith-number/JFNSJ4OG66L2B5PKZVZ5A6RO3J/events.json","paper":"https://pith.science/paper/JFNSJ4OG"},"agent_actions":{"view_html":"https://pith.science/pith/JFNSJ4OG66L2B5PKZVZ5A6RO3J","download_json":"https://pith.science/pith/JFNSJ4OG66L2B5PKZVZ5A6RO3J.json","view_paper":"https://pith.science/paper/JFNSJ4OG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9612207&json=true","fetch_graph":"https://pith.science/api/pith-number/JFNSJ4OG66L2B5PKZVZ5A6RO3J/graph.json","fetch_events":"https://pith.science/api/pith-number/JFNSJ4OG66L2B5PKZVZ5A6RO3J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JFNSJ4OG66L2B5PKZVZ5A6RO3J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JFNSJ4OG66L2B5PKZVZ5A6RO3J/action/storage_attestation","attest_author":"https://pith.science/pith/JFNSJ4OG66L2B5PKZVZ5A6RO3J/action/author_attestation","sign_citation":"https://pith.science/pith/JFNSJ4OG66L2B5PKZVZ5A6RO3J/action/citation_signature","submit_replication":"https://pith.science/pith/JFNSJ4OG66L2B5PKZVZ5A6RO3J/action/replication_record"}},"created_at":"2026-07-04T15:50:10.391656+00:00","updated_at":"2026-07-04T15:50:10.391656+00:00"}