{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:5NIFWWTB7WU7S4YEBLCK4B2ETV","short_pith_number":"pith:5NIFWWTB","schema_version":"1.0","canonical_sha256":"eb505b5a61fda9f973040ac4ae07449d53597bb76ff300d05029a5278c6e1774","source":{"kind":"arxiv","id":"hep-th/0106160","version":2},"attestation_state":"computed","paper":{"title":"N=2 Gauge Theories from Wrapped Five-branes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. L. Cotrone, A. Zaffaroni, F. Bigazzi","submitted_at":"2001-06-18T19:07:27Z","abstract_excerpt":"We present string duals of four dimensional N=2 pure SU(N) SYM theory. The theory is obtained as the low energy limit of D5-branes wrapped on non-trivial two-cycles. Using seven dimensional gauged supergravity and uplifting the result to ten dimensions, we obtain solutions corresponding to various points of the N=2 moduli space. The more symmetric solution may correspond to a point with rotationally invariant classical vevs. By turning on seven dimensional scalar fields, we find a solution corresponding to a linear distribution of vevs. Both solutions are conveniently studied with a D5-probe, "},"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/0106160","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-06-18T19:07:27Z","cross_cats_sorted":[],"title_canon_sha256":"df493fb6009c32109468e15954c7b811ca1c24029b9a2ac87f5e40f3f702e0c2","abstract_canon_sha256":"6c3658a5a310ad1d397e70d9e35caa58fad0ac7f1e942e4da4dcbebb6983aca2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:54.866924Z","signature_b64":"7N2ktCunYRpuCmVG6IeegmiBWO6AI45dzIAPQ/WJluKD/4QO84kVgIz++dAfb9z0lf+nTWfjZM3l1u5GFDdUDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eb505b5a61fda9f973040ac4ae07449d53597bb76ff300d05029a5278c6e1774","last_reissued_at":"2026-07-04T16:27:54.866415Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:54.866415Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"N=2 Gauge Theories from Wrapped Five-branes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. L. Cotrone, A. Zaffaroni, F. Bigazzi","submitted_at":"2001-06-18T19:07:27Z","abstract_excerpt":"We present string duals of four dimensional N=2 pure SU(N) SYM theory. The theory is obtained as the low energy limit of D5-branes wrapped on non-trivial two-cycles. Using seven dimensional gauged supergravity and uplifting the result to ten dimensions, we obtain solutions corresponding to various points of the N=2 moduli space. The more symmetric solution may correspond to a point with rotationally invariant classical vevs. By turning on seven dimensional scalar fields, we find a solution corresponding to a linear distribution of vevs. Both solutions are conveniently studied with a D5-probe, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0106160","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/0106160/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/0106160","created_at":"2026-07-04T16:27:54.866500+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0106160v2","created_at":"2026-07-04T16:27:54.866500+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0106160","created_at":"2026-07-04T16:27:54.866500+00:00"},{"alias_kind":"pith_short_12","alias_value":"5NIFWWTB7WU7","created_at":"2026-07-04T16:27:54.866500+00:00"},{"alias_kind":"pith_short_16","alias_value":"5NIFWWTB7WU7S4YE","created_at":"2026-07-04T16:27:54.866500+00:00"},{"alias_kind":"pith_short_8","alias_value":"5NIFWWTB","created_at":"2026-07-04T16:27:54.866500+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.18128","citing_title":"Supersymmetric AdS Solitons, Coulomb Branch Flows and Twisted Compactifications","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5NIFWWTB7WU7S4YEBLCK4B2ETV","json":"https://pith.science/pith/5NIFWWTB7WU7S4YEBLCK4B2ETV.json","graph_json":"https://pith.science/api/pith-number/5NIFWWTB7WU7S4YEBLCK4B2ETV/graph.json","events_json":"https://pith.science/api/pith-number/5NIFWWTB7WU7S4YEBLCK4B2ETV/events.json","paper":"https://pith.science/paper/5NIFWWTB"},"agent_actions":{"view_html":"https://pith.science/pith/5NIFWWTB7WU7S4YEBLCK4B2ETV","download_json":"https://pith.science/pith/5NIFWWTB7WU7S4YEBLCK4B2ETV.json","view_paper":"https://pith.science/paper/5NIFWWTB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0106160&json=true","fetch_graph":"https://pith.science/api/pith-number/5NIFWWTB7WU7S4YEBLCK4B2ETV/graph.json","fetch_events":"https://pith.science/api/pith-number/5NIFWWTB7WU7S4YEBLCK4B2ETV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5NIFWWTB7WU7S4YEBLCK4B2ETV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5NIFWWTB7WU7S4YEBLCK4B2ETV/action/storage_attestation","attest_author":"https://pith.science/pith/5NIFWWTB7WU7S4YEBLCK4B2ETV/action/author_attestation","sign_citation":"https://pith.science/pith/5NIFWWTB7WU7S4YEBLCK4B2ETV/action/citation_signature","submit_replication":"https://pith.science/pith/5NIFWWTB7WU7S4YEBLCK4B2ETV/action/replication_record"}},"created_at":"2026-07-04T16:27:54.866500+00:00","updated_at":"2026-07-04T16:27:54.866500+00:00"}