{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:TOXQY2M4Z3EYIOTI3XBR6LGGM7","short_pith_number":"pith:TOXQY2M4","schema_version":"1.0","canonical_sha256":"9baf0c699ccec9843a68ddc31f2cc667faa117b59aa2026f703e8bb35a7f501e","source":{"kind":"arxiv","id":"hep-th/9603042","version":1},"attestation_state":"computed","paper":{"title":"The Moduli Space of N=2 SUSY QCD and Duality in N=1 SUSY QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"M.R. Plesser, N. Seiberg, P.C. Argyres","submitted_at":"1996-03-07T20:01:29Z","abstract_excerpt":"We analyze in detail the moduli space of vacua of N=2 SUSY QCD with n_c colors and n_f flavors. The Coulomb branch has submanifolds with non-Abelian gauge symmetry. The massless quarks and gluons at these vacua are smoothly connected to the underlying elementary quarks and gluons. Upon breaking N=2 by an N=1 preserving mass term for the adjoint field the theory flows to N=1 SUSY QCD. Some of the massless quarks and gluons on the moduli space of the N=2 theory become the magnetic quarks and gluons of the N=1 theory. In this way we derive the duality in N=1 SUSY QCD by identifying its crucial bu"},"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/9603042","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-03-07T20:01:29Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ba03e474ffce8d162b6b631ff4fe6d9be7801dff83e9c93e8f242197070d8cf4","abstract_canon_sha256":"a21cf1d4b6b05d428d144a05ba4d9ef822c3dc96592700c8831d0efadbfd8d1e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:49:42.017029Z","signature_b64":"YY+Btx6DVMIw6JAYZ0GkVnNFvMejoSj0YGtWQB2/xtNQBFBh7oP0Vdq6DQf3EwiVL8T3lUFIu5kx6UDJ0fL6Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9baf0c699ccec9843a68ddc31f2cc667faa117b59aa2026f703e8bb35a7f501e","last_reissued_at":"2026-07-04T15:49:42.016680Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:49:42.016680Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Moduli Space of N=2 SUSY QCD and Duality in N=1 SUSY QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"M.R. Plesser, N. Seiberg, P.C. Argyres","submitted_at":"1996-03-07T20:01:29Z","abstract_excerpt":"We analyze in detail the moduli space of vacua of N=2 SUSY QCD with n_c colors and n_f flavors. The Coulomb branch has submanifolds with non-Abelian gauge symmetry. The massless quarks and gluons at these vacua are smoothly connected to the underlying elementary quarks and gluons. Upon breaking N=2 by an N=1 preserving mass term for the adjoint field the theory flows to N=1 SUSY QCD. Some of the massless quarks and gluons on the moduli space of the N=2 theory become the magnetic quarks and gluons of the N=1 theory. In this way we derive the duality in N=1 SUSY QCD by identifying its crucial bu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9603042","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9603042/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/9603042","created_at":"2026-07-04T15:49:42.016742+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9603042v1","created_at":"2026-07-04T15:49:42.016742+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9603042","created_at":"2026-07-04T15:49:42.016742+00:00"},{"alias_kind":"pith_short_12","alias_value":"TOXQY2M4Z3EY","created_at":"2026-07-04T15:49:42.016742+00:00"},{"alias_kind":"pith_short_16","alias_value":"TOXQY2M4Z3EYIOTI","created_at":"2026-07-04T15:49:42.016742+00:00"},{"alias_kind":"pith_short_8","alias_value":"TOXQY2M4","created_at":"2026-07-04T15:49:42.016742+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2607.01327","citing_title":"Algorithmic Dualization of Unitary Circular Quivers","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2412.03588","citing_title":"Spectral Networks: Bridging higher-rank Teichm\\\"uller theory and BPS states","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2502.01323","citing_title":"Quiver Yangians as Coulomb branch algebras","ref_index":35,"is_internal_anchor":true},{"citing_arxiv_id":"2604.27066","citing_title":"Perturbative Coulomb branches on $\\mathbb{R}^3\\times S^1$: the global D-term potential","ref_index":5,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TOXQY2M4Z3EYIOTI3XBR6LGGM7","json":"https://pith.science/pith/TOXQY2M4Z3EYIOTI3XBR6LGGM7.json","graph_json":"https://pith.science/api/pith-number/TOXQY2M4Z3EYIOTI3XBR6LGGM7/graph.json","events_json":"https://pith.science/api/pith-number/TOXQY2M4Z3EYIOTI3XBR6LGGM7/events.json","paper":"https://pith.science/paper/TOXQY2M4"},"agent_actions":{"view_html":"https://pith.science/pith/TOXQY2M4Z3EYIOTI3XBR6LGGM7","download_json":"https://pith.science/pith/TOXQY2M4Z3EYIOTI3XBR6LGGM7.json","view_paper":"https://pith.science/paper/TOXQY2M4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9603042&json=true","fetch_graph":"https://pith.science/api/pith-number/TOXQY2M4Z3EYIOTI3XBR6LGGM7/graph.json","fetch_events":"https://pith.science/api/pith-number/TOXQY2M4Z3EYIOTI3XBR6LGGM7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TOXQY2M4Z3EYIOTI3XBR6LGGM7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TOXQY2M4Z3EYIOTI3XBR6LGGM7/action/storage_attestation","attest_author":"https://pith.science/pith/TOXQY2M4Z3EYIOTI3XBR6LGGM7/action/author_attestation","sign_citation":"https://pith.science/pith/TOXQY2M4Z3EYIOTI3XBR6LGGM7/action/citation_signature","submit_replication":"https://pith.science/pith/TOXQY2M4Z3EYIOTI3XBR6LGGM7/action/replication_record"}},"created_at":"2026-07-04T15:49:42.016742+00:00","updated_at":"2026-07-04T15:49:42.016742+00:00"}