{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:UNGFG7QNY47IHKW4LZ2UKNHZAV","short_pith_number":"pith:UNGFG7QN","schema_version":"1.0","canonical_sha256":"a34c537e0dc73e83aadc5e754534f9056ff751d1791ea313fa22cb84b96593e2","source":{"kind":"arxiv","id":"hep-th/0311084","version":2},"attestation_state":"computed","paper":{"title":"Holomorphic D7-Branes and Flavored N=1 Gauge Theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Peter Ouyang","submitted_at":"2003-11-10T15:48:45Z","abstract_excerpt":"We consider D7-branes in the gauge theory/string theory correspondence, using a probe approximation. The D7-branes have four directions embedded holomorphically in a non-compact Calabi-Yau 3-fold (which for specificity we take to be the conifold) and their remaining four directions are parallel to a stack of D3-branes transverse to the Calabi-Yau space. The dual gauge theory, which has $\\mathcal{N}=1$ supersymmetry, contains quarks which transform in the fundamental representation of the gauge group, and we identify the interactions of these quarks in terms of a superpotential. By activating t"},"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/0311084","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-11-10T15:48:45Z","cross_cats_sorted":[],"title_canon_sha256":"2538ad7d6e4282a5ef5a3cbcfcd26e2e245b6d876636c89893ca3ea835bc1fdf","abstract_canon_sha256":"8d4e77158a6adf310dfe4622f0abc61312c045fc8e2b2bd161fd28b8c92e53b4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:45:46.447426Z","signature_b64":"MxUGWMuz3MYAuIGSfvJ7Pih3g0jLH3yhUfSic+7mauWEbe3XYvPcPn3DXIx+xExe1HogppPyfS+yC2LuiUtaBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a34c537e0dc73e83aadc5e754534f9056ff751d1791ea313fa22cb84b96593e2","last_reissued_at":"2026-07-04T15:45:46.447057Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:45:46.447057Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holomorphic D7-Branes and Flavored N=1 Gauge Theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Peter Ouyang","submitted_at":"2003-11-10T15:48:45Z","abstract_excerpt":"We consider D7-branes in the gauge theory/string theory correspondence, using a probe approximation. The D7-branes have four directions embedded holomorphically in a non-compact Calabi-Yau 3-fold (which for specificity we take to be the conifold) and their remaining four directions are parallel to a stack of D3-branes transverse to the Calabi-Yau space. The dual gauge theory, which has $\\mathcal{N}=1$ supersymmetry, contains quarks which transform in the fundamental representation of the gauge group, and we identify the interactions of these quarks in terms of a superpotential. By activating t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0311084","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/0311084/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/0311084","created_at":"2026-07-04T15:45:46.447119+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0311084v2","created_at":"2026-07-04T15:45:46.447119+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0311084","created_at":"2026-07-04T15:45:46.447119+00:00"},{"alias_kind":"pith_short_12","alias_value":"UNGFG7QNY47I","created_at":"2026-07-04T15:45:46.447119+00:00"},{"alias_kind":"pith_short_16","alias_value":"UNGFG7QNY47IHKW4","created_at":"2026-07-04T15:45:46.447119+00:00"},{"alias_kind":"pith_short_8","alias_value":"UNGFG7QN","created_at":"2026-07-04T15:45:46.447119+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.18988","citing_title":"Gravity, finite duality cascades and confinement","ref_index":42,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UNGFG7QNY47IHKW4LZ2UKNHZAV","json":"https://pith.science/pith/UNGFG7QNY47IHKW4LZ2UKNHZAV.json","graph_json":"https://pith.science/api/pith-number/UNGFG7QNY47IHKW4LZ2UKNHZAV/graph.json","events_json":"https://pith.science/api/pith-number/UNGFG7QNY47IHKW4LZ2UKNHZAV/events.json","paper":"https://pith.science/paper/UNGFG7QN"},"agent_actions":{"view_html":"https://pith.science/pith/UNGFG7QNY47IHKW4LZ2UKNHZAV","download_json":"https://pith.science/pith/UNGFG7QNY47IHKW4LZ2UKNHZAV.json","view_paper":"https://pith.science/paper/UNGFG7QN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0311084&json=true","fetch_graph":"https://pith.science/api/pith-number/UNGFG7QNY47IHKW4LZ2UKNHZAV/graph.json","fetch_events":"https://pith.science/api/pith-number/UNGFG7QNY47IHKW4LZ2UKNHZAV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UNGFG7QNY47IHKW4LZ2UKNHZAV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UNGFG7QNY47IHKW4LZ2UKNHZAV/action/storage_attestation","attest_author":"https://pith.science/pith/UNGFG7QNY47IHKW4LZ2UKNHZAV/action/author_attestation","sign_citation":"https://pith.science/pith/UNGFG7QNY47IHKW4LZ2UKNHZAV/action/citation_signature","submit_replication":"https://pith.science/pith/UNGFG7QNY47IHKW4LZ2UKNHZAV/action/replication_record"}},"created_at":"2026-07-04T15:45:46.447119+00:00","updated_at":"2026-07-04T15:45:46.447119+00:00"}