{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:E5RUZWJ7P33Q3TBVDOVEN3XCE2","short_pith_number":"pith:E5RUZWJ7","schema_version":"1.0","canonical_sha256":"27634cd93f7ef70dcc351baa46eee226b1e9d2c54478b045b80aca3ffc7711c0","source":{"kind":"arxiv","id":"hep-th/9909109","version":3},"attestation_state":"computed","paper":{"title":"An Orbifold of Type 0B Strings and Non-supersymmetric Gauge Theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Igor R. Klebanov, Nikita A. Nekrasov, Samson L. Shatashvili","submitted_at":"1999-09-15T19:35:09Z","abstract_excerpt":"We study a ${{\\IZ}}_2$ orbifold of Type 0B string theory by reflection of six of the coordinates (this theory may also be thought of as a ${{\\IZ}}_4$ orbifold of Type IIB string theory by a rotation by $\\pi$ in three independent planes). We show that the only massless mode localized on the fixed fourplane $\\IR^{3,1}$ is a U(1) gauge field. After introducing D3-branes parallel to the fixed fourplane we find non-supersymmetric non-abelian gauge theories on their worldvolume. One of our results is that the theory on equal numbers of electric and magnetic D3-branes placed at the fourplane is the $"},"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/9909109","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-09-15T19:35:09Z","cross_cats_sorted":[],"title_canon_sha256":"988a77e545fc9aef77d5d16fb3e2502b0c01d51a041068c4c0b0f413ff2551c7","abstract_canon_sha256":"826e6defe0957fcbfc48165e855aaad94787c0ff977725227fa603f2cf11f92b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:14:57.774862Z","signature_b64":"OAWuMereuczUf3PdO44p9xLH7ep+Ci2AHWsHOTzZQMFBxn1U40h4oxM1Yh9PVb5kAdTtf38dsBYNwDIb71x6Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"27634cd93f7ef70dcc351baa46eee226b1e9d2c54478b045b80aca3ffc7711c0","last_reissued_at":"2026-07-04T16:14:57.774471Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:14:57.774471Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An Orbifold of Type 0B Strings and Non-supersymmetric Gauge Theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Igor R. Klebanov, Nikita A. Nekrasov, Samson L. Shatashvili","submitted_at":"1999-09-15T19:35:09Z","abstract_excerpt":"We study a ${{\\IZ}}_2$ orbifold of Type 0B string theory by reflection of six of the coordinates (this theory may also be thought of as a ${{\\IZ}}_4$ orbifold of Type IIB string theory by a rotation by $\\pi$ in three independent planes). We show that the only massless mode localized on the fixed fourplane $\\IR^{3,1}$ is a U(1) gauge field. After introducing D3-branes parallel to the fixed fourplane we find non-supersymmetric non-abelian gauge theories on their worldvolume. One of our results is that the theory on equal numbers of electric and magnetic D3-branes placed at the fourplane is the $"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9909109","kind":"arxiv","version":3},"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/9909109/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/9909109","created_at":"2026-07-04T16:14:57.774531+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9909109v3","created_at":"2026-07-04T16:14:57.774531+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9909109","created_at":"2026-07-04T16:14:57.774531+00:00"},{"alias_kind":"pith_short_12","alias_value":"E5RUZWJ7P33Q","created_at":"2026-07-04T16:14:57.774531+00:00"},{"alias_kind":"pith_short_16","alias_value":"E5RUZWJ7P33Q3TBV","created_at":"2026-07-04T16:14:57.774531+00:00"},{"alias_kind":"pith_short_8","alias_value":"E5RUZWJ7","created_at":"2026-07-04T16:14:57.774531+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.04805","citing_title":"GSO projections via SPT phases","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/E5RUZWJ7P33Q3TBVDOVEN3XCE2","json":"https://pith.science/pith/E5RUZWJ7P33Q3TBVDOVEN3XCE2.json","graph_json":"https://pith.science/api/pith-number/E5RUZWJ7P33Q3TBVDOVEN3XCE2/graph.json","events_json":"https://pith.science/api/pith-number/E5RUZWJ7P33Q3TBVDOVEN3XCE2/events.json","paper":"https://pith.science/paper/E5RUZWJ7"},"agent_actions":{"view_html":"https://pith.science/pith/E5RUZWJ7P33Q3TBVDOVEN3XCE2","download_json":"https://pith.science/pith/E5RUZWJ7P33Q3TBVDOVEN3XCE2.json","view_paper":"https://pith.science/paper/E5RUZWJ7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9909109&json=true","fetch_graph":"https://pith.science/api/pith-number/E5RUZWJ7P33Q3TBVDOVEN3XCE2/graph.json","fetch_events":"https://pith.science/api/pith-number/E5RUZWJ7P33Q3TBVDOVEN3XCE2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/E5RUZWJ7P33Q3TBVDOVEN3XCE2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/E5RUZWJ7P33Q3TBVDOVEN3XCE2/action/storage_attestation","attest_author":"https://pith.science/pith/E5RUZWJ7P33Q3TBVDOVEN3XCE2/action/author_attestation","sign_citation":"https://pith.science/pith/E5RUZWJ7P33Q3TBVDOVEN3XCE2/action/citation_signature","submit_replication":"https://pith.science/pith/E5RUZWJ7P33Q3TBVDOVEN3XCE2/action/replication_record"}},"created_at":"2026-07-04T16:14:57.774531+00:00","updated_at":"2026-07-04T16:14:57.774531+00:00"}