{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:4ZR2P4MLXU6ZYWRFPIAVGMRICG","short_pith_number":"pith:4ZR2P4ML","schema_version":"1.0","canonical_sha256":"e663a7f18bbd3d9c5a257a0153322811811c6c40520e9c954d64788072073ac1","source":{"kind":"arxiv","id":"hep-th/9912066","version":3},"attestation_state":"computed","paper":{"title":"Self-Duality of Various Chiral Boson Actions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"H. J. W. Mueller-Kirsten, Yan-Gang Miao","submitted_at":"1999-12-08T10:57:54Z","abstract_excerpt":"The duality symmetries of various chiral boson actions are investigated using D=2 and D=6 space-time dimensions as examples. These actions involve the Siegel, Floreanini-Jackiw, Srivastava and Pasti-Sorokin-Tonin formulations. We discover that the Siegel, Floreanini-Jackiw and Pasti-Sorokin-Tonin actions have self-duality with respect to a common anti-dualization of chiral boson fields in D=2 and D=6 dimensions, respectively, while the Srivastava action is self-dual with respect to a generalized dualization of chiral boson fields. Moreover, the action of the Floreanini-Jackiw chiral bosons int"},"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/9912066","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-12-08T10:57:54Z","cross_cats_sorted":[],"title_canon_sha256":"f0c77818a2eb3769a033f64261de727736621143fa7aed5220556f698bf95d07","abstract_canon_sha256":"175cac11b163aefbd8426b7767c446886d4c8a80593193169b4d06616a545d30"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:15:04.321279Z","signature_b64":"D5JkkOQtssQOT/a0oaDIGf4T6ta206ub3VevQFf2F3wOqJOqiw5VlWDrCnciBzqaZWTjD4TzWkSokFhnZC8+AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e663a7f18bbd3d9c5a257a0153322811811c6c40520e9c954d64788072073ac1","last_reissued_at":"2026-07-04T16:15:04.320888Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:15:04.320888Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Self-Duality of Various Chiral Boson Actions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"H. J. W. Mueller-Kirsten, Yan-Gang Miao","submitted_at":"1999-12-08T10:57:54Z","abstract_excerpt":"The duality symmetries of various chiral boson actions are investigated using D=2 and D=6 space-time dimensions as examples. These actions involve the Siegel, Floreanini-Jackiw, Srivastava and Pasti-Sorokin-Tonin formulations. We discover that the Siegel, Floreanini-Jackiw and Pasti-Sorokin-Tonin actions have self-duality with respect to a common anti-dualization of chiral boson fields in D=2 and D=6 dimensions, respectively, while the Srivastava action is self-dual with respect to a generalized dualization of chiral boson fields. Moreover, the action of the Floreanini-Jackiw chiral bosons int"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9912066","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/9912066/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/9912066","created_at":"2026-07-04T16:15:04.320946+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9912066v3","created_at":"2026-07-04T16:15:04.320946+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9912066","created_at":"2026-07-04T16:15:04.320946+00:00"},{"alias_kind":"pith_short_12","alias_value":"4ZR2P4MLXU6Z","created_at":"2026-07-04T16:15:04.320946+00:00"},{"alias_kind":"pith_short_16","alias_value":"4ZR2P4MLXU6ZYWRF","created_at":"2026-07-04T16:15:04.320946+00:00"},{"alias_kind":"pith_short_8","alias_value":"4ZR2P4ML","created_at":"2026-07-04T16:15:04.320946+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.09159","citing_title":"A (1+1)-dimensional Lifshitz Weyl Anomaly From a Schr$\\mathrm{\\ddot{o}}$dinger-invariant Non-relativistic Chern-Simons Action","ref_index":47,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4ZR2P4MLXU6ZYWRFPIAVGMRICG","json":"https://pith.science/pith/4ZR2P4MLXU6ZYWRFPIAVGMRICG.json","graph_json":"https://pith.science/api/pith-number/4ZR2P4MLXU6ZYWRFPIAVGMRICG/graph.json","events_json":"https://pith.science/api/pith-number/4ZR2P4MLXU6ZYWRFPIAVGMRICG/events.json","paper":"https://pith.science/paper/4ZR2P4ML"},"agent_actions":{"view_html":"https://pith.science/pith/4ZR2P4MLXU6ZYWRFPIAVGMRICG","download_json":"https://pith.science/pith/4ZR2P4MLXU6ZYWRFPIAVGMRICG.json","view_paper":"https://pith.science/paper/4ZR2P4ML","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9912066&json=true","fetch_graph":"https://pith.science/api/pith-number/4ZR2P4MLXU6ZYWRFPIAVGMRICG/graph.json","fetch_events":"https://pith.science/api/pith-number/4ZR2P4MLXU6ZYWRFPIAVGMRICG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4ZR2P4MLXU6ZYWRFPIAVGMRICG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4ZR2P4MLXU6ZYWRFPIAVGMRICG/action/storage_attestation","attest_author":"https://pith.science/pith/4ZR2P4MLXU6ZYWRFPIAVGMRICG/action/author_attestation","sign_citation":"https://pith.science/pith/4ZR2P4MLXU6ZYWRFPIAVGMRICG/action/citation_signature","submit_replication":"https://pith.science/pith/4ZR2P4MLXU6ZYWRFPIAVGMRICG/action/replication_record"}},"created_at":"2026-07-04T16:15:04.320946+00:00","updated_at":"2026-07-04T16:15:04.320946+00:00"}