{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:MQXXW3XZNNG5XXZBDENITCB5CO","short_pith_number":"pith:MQXXW3XZ","schema_version":"1.0","canonical_sha256":"642f7b6ef96b4ddbdf21191a89883d13abfa9221524fc70ca751ae255942a3df","source":{"kind":"arxiv","id":"hep-th/0007231","version":1},"attestation_state":"computed","paper":{"title":"Nonlinear Self-Duality and Supersymmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Sergei M. Kuzenko, Stefan Theisen (University of Munich)","submitted_at":"2000-07-28T16:14:01Z","abstract_excerpt":"We review self-duality of nonlinear electrodynamics and its extension to several Abelian gauge fields coupled to scalars. We then describe self-duality in supersymmetric models, both N = 1 and N = 2. The self-duality equations, which have to be satisfied by the action of any self-dual system, are found and solutions are discussed. One important example is the Born-Infeld action. We explain why the N = 2 supersymmetric actions proposed so far are not the correct world-volume actions for D3 branes in d = 6."},"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/0007231","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2000-07-28T16:14:01Z","cross_cats_sorted":[],"title_canon_sha256":"e4192965ce51048c77e60ec169f00abc06f12ac951a4589853e6cd89002671fb","abstract_canon_sha256":"de003941e4fbb78563583b9d044a33bdb06c13252a2dbed9d08943d6811371ff"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:55.334948Z","signature_b64":"ACTqGA3DQO+AkJg7/ADtmKxE5f9LgzXRhl4oM8oNRs0VZyHyy77PSesC3bNLuxpqaCQC/OPLTe2rTUFQal/OCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"642f7b6ef96b4ddbdf21191a89883d13abfa9221524fc70ca751ae255942a3df","last_reissued_at":"2026-05-18T01:38:55.334203Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:55.334203Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonlinear Self-Duality and Supersymmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Sergei M. Kuzenko, Stefan Theisen (University of Munich)","submitted_at":"2000-07-28T16:14:01Z","abstract_excerpt":"We review self-duality of nonlinear electrodynamics and its extension to several Abelian gauge fields coupled to scalars. We then describe self-duality in supersymmetric models, both N = 1 and N = 2. The self-duality equations, which have to be satisfied by the action of any self-dual system, are found and solutions are discussed. One important example is the Born-Infeld action. We explain why the N = 2 supersymmetric actions proposed so far are not the correct world-volume actions for D3 branes in d = 6."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0007231","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":"hep-th/0007231","created_at":"2026-05-18T01:38:55.334333+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0007231v1","created_at":"2026-05-18T01:38:55.334333+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0007231","created_at":"2026-05-18T01:38:55.334333+00:00"},{"alias_kind":"pith_short_12","alias_value":"MQXXW3XZNNG5","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"MQXXW3XZNNG5XXZB","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"MQXXW3XZ","created_at":"2026-05-18T12:25:50.254431+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2605.06193","citing_title":"Causal self-dual nonlinear electrodynamics from the Born-Infeld theory","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2606.00536","citing_title":"The Triple $T\\bar{T}$-Like Flow in Quantum Field Theories: Irrelevant, Marginal, and Relevant","ref_index":39,"is_internal_anchor":true},{"citing_arxiv_id":"2601.19339","citing_title":"Heat kernel approach to the one-loop effective action for nonlinear electrodynamics","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2601.19339","citing_title":"Heat kernel approach to the one-loop effective action for nonlinear electrodynamics","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2605.06193","citing_title":"Causal self-dual nonlinear electrodynamics from the Born-Infeld theory","ref_index":9,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MQXXW3XZNNG5XXZBDENITCB5CO","json":"https://pith.science/pith/MQXXW3XZNNG5XXZBDENITCB5CO.json","graph_json":"https://pith.science/api/pith-number/MQXXW3XZNNG5XXZBDENITCB5CO/graph.json","events_json":"https://pith.science/api/pith-number/MQXXW3XZNNG5XXZBDENITCB5CO/events.json","paper":"https://pith.science/paper/MQXXW3XZ"},"agent_actions":{"view_html":"https://pith.science/pith/MQXXW3XZNNG5XXZBDENITCB5CO","download_json":"https://pith.science/pith/MQXXW3XZNNG5XXZBDENITCB5CO.json","view_paper":"https://pith.science/paper/MQXXW3XZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0007231&json=true","fetch_graph":"https://pith.science/api/pith-number/MQXXW3XZNNG5XXZBDENITCB5CO/graph.json","fetch_events":"https://pith.science/api/pith-number/MQXXW3XZNNG5XXZBDENITCB5CO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MQXXW3XZNNG5XXZBDENITCB5CO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MQXXW3XZNNG5XXZBDENITCB5CO/action/storage_attestation","attest_author":"https://pith.science/pith/MQXXW3XZNNG5XXZBDENITCB5CO/action/author_attestation","sign_citation":"https://pith.science/pith/MQXXW3XZNNG5XXZBDENITCB5CO/action/citation_signature","submit_replication":"https://pith.science/pith/MQXXW3XZNNG5XXZBDENITCB5CO/action/replication_record"}},"created_at":"2026-05-18T01:38:55.334333+00:00","updated_at":"2026-05-18T01:38:55.334333+00:00"}