{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:UOKHY2X2FRT3ASS6TQ65BUUGAX","short_pith_number":"pith:UOKHY2X2","schema_version":"1.0","canonical_sha256":"a3947c6afa2c67b04a5e9c3dd0d28605d914322a88cb781bc571ac00dfb0a4bd","source":{"kind":"arxiv","id":"hep-th/0307287","version":2},"attestation_state":"computed","paper":{"title":"Nonabelian Superconductors: Vortices and Confinement in ${\\cal N}=2$ SQCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alexei Yung, Jarah Evslin, Kenichi Konishi, Roberto Auzzi, Stefano Bolognesi","submitted_at":"2003-07-30T06:43:20Z","abstract_excerpt":"We study nonabelian vortices (flux tubes) in SU(N) gauge theories, which are responsible for the confinement of (nonabelian) magnetic monopoles. In particular a detailed analysis is given of ${\\cal N}=2$ SQCD with gauge group SU(3) deformed by a small adjoint chiral multiplet mass. Tuning the bare quark masses (which we take to be large) to a common value $m$, we consider a particular vacuum of this theory in which an SU(2) subgroup of the gauge group remains unbroken. We consider $5 \\ge N_f \\ge 4$ flavors so that the SU(2) sub-sector remains non asymptotically free: the vortices carrying nona"},"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/0307287","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-07-30T06:43:20Z","cross_cats_sorted":[],"title_canon_sha256":"a323f7317075eba30878a36e9ccdcfd5860c48e2e06834ba12721dbfc5913ecc","abstract_canon_sha256":"7c206ddaad87b2c27b1adafc43f2da5f9081f9fc613bdfe5cdf98321d4aa61a9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:29:26.809065Z","signature_b64":"uF0J6HOkzqFlzix26M+WSCY2ceDghOFRV9Qpkn1V6BgocTKfCoY4rr8Z0MUsxAmUS8tdLHeLODxZeDWexuJaBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a3947c6afa2c67b04a5e9c3dd0d28605d914322a88cb781bc571ac00dfb0a4bd","last_reissued_at":"2026-07-04T17:29:26.808581Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:29:26.808581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonabelian Superconductors: Vortices and Confinement in ${\\cal N}=2$ SQCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alexei Yung, Jarah Evslin, Kenichi Konishi, Roberto Auzzi, Stefano Bolognesi","submitted_at":"2003-07-30T06:43:20Z","abstract_excerpt":"We study nonabelian vortices (flux tubes) in SU(N) gauge theories, which are responsible for the confinement of (nonabelian) magnetic monopoles. In particular a detailed analysis is given of ${\\cal N}=2$ SQCD with gauge group SU(3) deformed by a small adjoint chiral multiplet mass. Tuning the bare quark masses (which we take to be large) to a common value $m$, we consider a particular vacuum of this theory in which an SU(2) subgroup of the gauge group remains unbroken. We consider $5 \\ge N_f \\ge 4$ flavors so that the SU(2) sub-sector remains non asymptotically free: the vortices carrying nona"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0307287","kind":"arxiv","version":2},"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/0307287/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/0307287","created_at":"2026-07-04T17:29:26.808638+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0307287v2","created_at":"2026-07-04T17:29:26.808638+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0307287","created_at":"2026-07-04T17:29:26.808638+00:00"},{"alias_kind":"pith_short_12","alias_value":"UOKHY2X2FRT3","created_at":"2026-07-04T17:29:26.808638+00:00"},{"alias_kind":"pith_short_16","alias_value":"UOKHY2X2FRT3ASS6","created_at":"2026-07-04T17:29:26.808638+00:00"},{"alias_kind":"pith_short_8","alias_value":"UOKHY2X2","created_at":"2026-07-04T17:29:26.808638+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.21755","citing_title":"Universalities of Defects in Quantum Field Theories","ref_index":140,"is_internal_anchor":true},{"citing_arxiv_id":"2605.06550","citing_title":"Hadrons in $\\mathcal{N}=2$ supersymmetric QCD from non-Abelian string on 2D black hole","ref_index":2,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UOKHY2X2FRT3ASS6TQ65BUUGAX","json":"https://pith.science/pith/UOKHY2X2FRT3ASS6TQ65BUUGAX.json","graph_json":"https://pith.science/api/pith-number/UOKHY2X2FRT3ASS6TQ65BUUGAX/graph.json","events_json":"https://pith.science/api/pith-number/UOKHY2X2FRT3ASS6TQ65BUUGAX/events.json","paper":"https://pith.science/paper/UOKHY2X2"},"agent_actions":{"view_html":"https://pith.science/pith/UOKHY2X2FRT3ASS6TQ65BUUGAX","download_json":"https://pith.science/pith/UOKHY2X2FRT3ASS6TQ65BUUGAX.json","view_paper":"https://pith.science/paper/UOKHY2X2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0307287&json=true","fetch_graph":"https://pith.science/api/pith-number/UOKHY2X2FRT3ASS6TQ65BUUGAX/graph.json","fetch_events":"https://pith.science/api/pith-number/UOKHY2X2FRT3ASS6TQ65BUUGAX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UOKHY2X2FRT3ASS6TQ65BUUGAX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UOKHY2X2FRT3ASS6TQ65BUUGAX/action/storage_attestation","attest_author":"https://pith.science/pith/UOKHY2X2FRT3ASS6TQ65BUUGAX/action/author_attestation","sign_citation":"https://pith.science/pith/UOKHY2X2FRT3ASS6TQ65BUUGAX/action/citation_signature","submit_replication":"https://pith.science/pith/UOKHY2X2FRT3ASS6TQ65BUUGAX/action/replication_record"}},"created_at":"2026-07-04T17:29:26.808638+00:00","updated_at":"2026-07-04T17:29:26.808638+00:00"}