{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:MXR3QK453VU242NMWXL6SBP6FX","short_pith_number":"pith:MXR3QK45","schema_version":"1.0","canonical_sha256":"65e3b82b9ddd69ae69acb5d7e905fe2dc8e466e017280fd14e50b9db6b043e6f","source":{"kind":"arxiv","id":"hep-th/9803214","version":2},"attestation_state":"computed","paper":{"title":"Gauge Theories from Orientifolds and Large N Limit","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Zurab Kakushadze","submitted_at":"1998-03-25T22:52:39Z","abstract_excerpt":"Extending the recent work in hep-th/9803076, we consider string perturbative expansion in the presence of D-branes and orientifold planes imbedded in orbifolded space-time. In the $\\alpha'\\to 0$ limit the weak coupling string perturbative expansion maps to `t Hooft's large N expansion. We focus on four dimensional ${\\cal N}=1,2,4$ supersymmetric theories, and also discuss possible extensions to ${\\cal N}=0$ cases. Utilizing the string theory perturbation techniques we show that computation of any M-point correlation function in these theories reduces to the corresponding computation in the par"},"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/9803214","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-03-25T22:52:39Z","cross_cats_sorted":[],"title_canon_sha256":"fc7912165492e20511c48526f844942223613ce215ddb772ad05d94cc4ac47cb","abstract_canon_sha256":"0cd18be4214c7eaf558c4d76e9225550e047bbdeea60ae6d3ec1ee19b73dc171"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:09:44.567060Z","signature_b64":"9SIhkAvqoVQ/M9umDPRxcSTW4WHLAbG6ERtCK56oQbk1R/4ilcEMrjJnyQqiD45LwK9paw6oG8rDYg8OQrSyCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"65e3b82b9ddd69ae69acb5d7e905fe2dc8e466e017280fd14e50b9db6b043e6f","last_reissued_at":"2026-07-04T16:09:44.566696Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:09:44.566696Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gauge Theories from Orientifolds and Large N Limit","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Zurab Kakushadze","submitted_at":"1998-03-25T22:52:39Z","abstract_excerpt":"Extending the recent work in hep-th/9803076, we consider string perturbative expansion in the presence of D-branes and orientifold planes imbedded in orbifolded space-time. In the $\\alpha'\\to 0$ limit the weak coupling string perturbative expansion maps to `t Hooft's large N expansion. We focus on four dimensional ${\\cal N}=1,2,4$ supersymmetric theories, and also discuss possible extensions to ${\\cal N}=0$ cases. Utilizing the string theory perturbation techniques we show that computation of any M-point correlation function in these theories reduces to the corresponding computation in the par"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9803214","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/9803214/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/9803214","created_at":"2026-07-04T16:09:44.566758+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9803214v2","created_at":"2026-07-04T16:09:44.566758+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9803214","created_at":"2026-07-04T16:09:44.566758+00:00"},{"alias_kind":"pith_short_12","alias_value":"MXR3QK453VU2","created_at":"2026-07-04T16:09:44.566758+00:00"},{"alias_kind":"pith_short_16","alias_value":"MXR3QK453VU242NM","created_at":"2026-07-04T16:09:44.566758+00:00"},{"alias_kind":"pith_short_8","alias_value":"MXR3QK45","created_at":"2026-07-04T16:09:44.566758+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.13910","citing_title":"Localization and wall-crossing of giant graviton expansions in AdS$_5$","ref_index":37,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MXR3QK453VU242NMWXL6SBP6FX","json":"https://pith.science/pith/MXR3QK453VU242NMWXL6SBP6FX.json","graph_json":"https://pith.science/api/pith-number/MXR3QK453VU242NMWXL6SBP6FX/graph.json","events_json":"https://pith.science/api/pith-number/MXR3QK453VU242NMWXL6SBP6FX/events.json","paper":"https://pith.science/paper/MXR3QK45"},"agent_actions":{"view_html":"https://pith.science/pith/MXR3QK453VU242NMWXL6SBP6FX","download_json":"https://pith.science/pith/MXR3QK453VU242NMWXL6SBP6FX.json","view_paper":"https://pith.science/paper/MXR3QK45","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9803214&json=true","fetch_graph":"https://pith.science/api/pith-number/MXR3QK453VU242NMWXL6SBP6FX/graph.json","fetch_events":"https://pith.science/api/pith-number/MXR3QK453VU242NMWXL6SBP6FX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MXR3QK453VU242NMWXL6SBP6FX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MXR3QK453VU242NMWXL6SBP6FX/action/storage_attestation","attest_author":"https://pith.science/pith/MXR3QK453VU242NMWXL6SBP6FX/action/author_attestation","sign_citation":"https://pith.science/pith/MXR3QK453VU242NMWXL6SBP6FX/action/citation_signature","submit_replication":"https://pith.science/pith/MXR3QK453VU242NMWXL6SBP6FX/action/replication_record"}},"created_at":"2026-07-04T16:09:44.566758+00:00","updated_at":"2026-07-04T16:09:44.566758+00:00"}