{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:HHJHPJUBGD5NRAB3CUD5G2OYX2","short_pith_number":"pith:HHJHPJUB","schema_version":"1.0","canonical_sha256":"39d277a68130fad8803b1507d369d8bea147f4ef24b4c7707048922883ca395e","source":{"kind":"arxiv","id":"1406.6287","version":1},"attestation_state":"computed","paper":{"title":"Generalized Yang-Mills theory and the D-brane effective action","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Athanasios Chatzistavrakidis, Fridrik Freyr Gautason","submitted_at":"2014-06-24T16:02:44Z","abstract_excerpt":"Non-abelian gauge theories in the context of generalized complex geometry are discussed. The generalized connection naturally contains standard gauge and scalar fields, unified in a purely geometric way. We define the corresponding Yang-Mills theory on particular subbundles of a Courant algebroid, known as Dirac structures, where the generalized curvature is a tensor. Different Dirac structures correspond to different known theories, such as the bosonic sector of maximally supersymmetric Yang-Mills in ten and four dimensions and reduced matrix models. Furthermore, we revisit the non-abelian wo"},"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":"1406.6287","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-24T16:02:44Z","cross_cats_sorted":[],"title_canon_sha256":"ff32e5eb83f7eaaa920860e6771c25c16aedc466bf70f1efc42f41d3440de5f8","abstract_canon_sha256":"9d4447cf2b7dfccbb0e5e6dc2f6a1e0dc2c0bc7c4174d17585f59e896b9001dc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:49:03.722342Z","signature_b64":"bo8Gda5/FHKd8oZR//3Vzon6ivAlsYPMojJhpHMSvKbekFDmOWz7U22xn1w/jzQjPRJuVb4H7e355mYY4TcaAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"39d277a68130fad8803b1507d369d8bea147f4ef24b4c7707048922883ca395e","last_reissued_at":"2026-05-18T02:49:03.721896Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:49:03.721896Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Generalized Yang-Mills theory and the D-brane effective action","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Athanasios Chatzistavrakidis, Fridrik Freyr Gautason","submitted_at":"2014-06-24T16:02:44Z","abstract_excerpt":"Non-abelian gauge theories in the context of generalized complex geometry are discussed. The generalized connection naturally contains standard gauge and scalar fields, unified in a purely geometric way. We define the corresponding Yang-Mills theory on particular subbundles of a Courant algebroid, known as Dirac structures, where the generalized curvature is a tensor. Different Dirac structures correspond to different known theories, such as the bosonic sector of maximally supersymmetric Yang-Mills in ten and four dimensions and reduced matrix models. Furthermore, we revisit the non-abelian wo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.6287","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1406.6287","created_at":"2026-05-18T02:49:03.721967+00:00"},{"alias_kind":"arxiv_version","alias_value":"1406.6287v1","created_at":"2026-05-18T02:49:03.721967+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.6287","created_at":"2026-05-18T02:49:03.721967+00:00"},{"alias_kind":"pith_short_12","alias_value":"HHJHPJUBGD5N","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_16","alias_value":"HHJHPJUBGD5NRAB3","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_8","alias_value":"HHJHPJUB","created_at":"2026-05-18T12:28:30.664211+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HHJHPJUBGD5NRAB3CUD5G2OYX2","json":"https://pith.science/pith/HHJHPJUBGD5NRAB3CUD5G2OYX2.json","graph_json":"https://pith.science/api/pith-number/HHJHPJUBGD5NRAB3CUD5G2OYX2/graph.json","events_json":"https://pith.science/api/pith-number/HHJHPJUBGD5NRAB3CUD5G2OYX2/events.json","paper":"https://pith.science/paper/HHJHPJUB"},"agent_actions":{"view_html":"https://pith.science/pith/HHJHPJUBGD5NRAB3CUD5G2OYX2","download_json":"https://pith.science/pith/HHJHPJUBGD5NRAB3CUD5G2OYX2.json","view_paper":"https://pith.science/paper/HHJHPJUB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1406.6287&json=true","fetch_graph":"https://pith.science/api/pith-number/HHJHPJUBGD5NRAB3CUD5G2OYX2/graph.json","fetch_events":"https://pith.science/api/pith-number/HHJHPJUBGD5NRAB3CUD5G2OYX2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HHJHPJUBGD5NRAB3CUD5G2OYX2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HHJHPJUBGD5NRAB3CUD5G2OYX2/action/storage_attestation","attest_author":"https://pith.science/pith/HHJHPJUBGD5NRAB3CUD5G2OYX2/action/author_attestation","sign_citation":"https://pith.science/pith/HHJHPJUBGD5NRAB3CUD5G2OYX2/action/citation_signature","submit_replication":"https://pith.science/pith/HHJHPJUBGD5NRAB3CUD5G2OYX2/action/replication_record"}},"created_at":"2026-05-18T02:49:03.721967+00:00","updated_at":"2026-05-18T02:49:03.721967+00:00"}