{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:KPBHLQFQYN4LMLKSS3UNHSGUOQ","short_pith_number":"pith:KPBHLQFQ","schema_version":"1.0","canonical_sha256":"53c275c0b0c378b62d5296e8d3c8d4743b0d219db6fc6a9a81f483c1a1743e19","source":{"kind":"arxiv","id":"hep-th/9812090","version":3},"attestation_state":"computed","paper":{"title":"Partial duality in SU(N) Yang-Mills theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Antti J. Niemi, L. Faddeev","submitted_at":"1998-12-10T20:39:26Z","abstract_excerpt":"Recently we have proposed a set of variables for describing the infrared limit of four dimensional SU(2) Yang-Mills theory. here we extend these variables to the general case of four dimensional SU(N) Yang-Mills theory. We find that the SU(N) connection A decomposes according to irreducible representations of SO(N-1) and the curvature two-form F is related to the symplectic Kirillov two forms that characterize irreducible representations of SU(N). We propose a general class of nonlinear chiral models that may describe stable, soliton-like configurations with nontrivial topological numbers."},"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/9812090","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-12-10T20:39:26Z","cross_cats_sorted":[],"title_canon_sha256":"49dd91fb75ed6ee493cc169d0d40ec8a5f4cf2b1ce88035a098ca7f7fb42b181","abstract_canon_sha256":"f249ced948ea99d29a461e364192dd84eb30180d32ea0cfb797b35969ca766ee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:10:06.106207Z","signature_b64":"8QGF2dB78Z/761W/0FXbZ1sNTKqMvfo4yZk4ag08qqgQRtgQMKtroZzzD+HgIfF8A8XFVCZVZnlfsbDEecXrBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53c275c0b0c378b62d5296e8d3c8d4743b0d219db6fc6a9a81f483c1a1743e19","last_reissued_at":"2026-07-04T16:10:06.105797Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:10:06.105797Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Partial duality in SU(N) Yang-Mills theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Antti J. Niemi, L. Faddeev","submitted_at":"1998-12-10T20:39:26Z","abstract_excerpt":"Recently we have proposed a set of variables for describing the infrared limit of four dimensional SU(2) Yang-Mills theory. here we extend these variables to the general case of four dimensional SU(N) Yang-Mills theory. We find that the SU(N) connection A decomposes according to irreducible representations of SO(N-1) and the curvature two-form F is related to the symplectic Kirillov two forms that characterize irreducible representations of SU(N). We propose a general class of nonlinear chiral models that may describe stable, soliton-like configurations with nontrivial topological numbers."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9812090","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/9812090/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/9812090","created_at":"2026-07-04T16:10:06.105857+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9812090v3","created_at":"2026-07-04T16:10:06.105857+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9812090","created_at":"2026-07-04T16:10:06.105857+00:00"},{"alias_kind":"pith_short_12","alias_value":"KPBHLQFQYN4L","created_at":"2026-07-04T16:10:06.105857+00:00"},{"alias_kind":"pith_short_16","alias_value":"KPBHLQFQYN4LMLKS","created_at":"2026-07-04T16:10:06.105857+00:00"},{"alias_kind":"pith_short_8","alias_value":"KPBHLQFQ","created_at":"2026-07-04T16:10:06.105857+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.29668","citing_title":"Understanding Color Confinement through Quantum Reference Frames and Relational Observables","ref_index":50,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KPBHLQFQYN4LMLKSS3UNHSGUOQ","json":"https://pith.science/pith/KPBHLQFQYN4LMLKSS3UNHSGUOQ.json","graph_json":"https://pith.science/api/pith-number/KPBHLQFQYN4LMLKSS3UNHSGUOQ/graph.json","events_json":"https://pith.science/api/pith-number/KPBHLQFQYN4LMLKSS3UNHSGUOQ/events.json","paper":"https://pith.science/paper/KPBHLQFQ"},"agent_actions":{"view_html":"https://pith.science/pith/KPBHLQFQYN4LMLKSS3UNHSGUOQ","download_json":"https://pith.science/pith/KPBHLQFQYN4LMLKSS3UNHSGUOQ.json","view_paper":"https://pith.science/paper/KPBHLQFQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9812090&json=true","fetch_graph":"https://pith.science/api/pith-number/KPBHLQFQYN4LMLKSS3UNHSGUOQ/graph.json","fetch_events":"https://pith.science/api/pith-number/KPBHLQFQYN4LMLKSS3UNHSGUOQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KPBHLQFQYN4LMLKSS3UNHSGUOQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KPBHLQFQYN4LMLKSS3UNHSGUOQ/action/storage_attestation","attest_author":"https://pith.science/pith/KPBHLQFQYN4LMLKSS3UNHSGUOQ/action/author_attestation","sign_citation":"https://pith.science/pith/KPBHLQFQYN4LMLKSS3UNHSGUOQ/action/citation_signature","submit_replication":"https://pith.science/pith/KPBHLQFQYN4LMLKSS3UNHSGUOQ/action/replication_record"}},"created_at":"2026-07-04T16:10:06.105857+00:00","updated_at":"2026-07-04T16:10:06.105857+00:00"}