{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:RZXNFS6B6SMEX2FYROCKYK6WWW","short_pith_number":"pith:RZXNFS6B","schema_version":"1.0","canonical_sha256":"8e6ed2cbc1f4984be8b88b84ac2bd6b5b8326d93e6120aed44748174b3010de4","source":{"kind":"arxiv","id":"hep-th/0403149","version":4},"attestation_state":"computed","paper":{"title":"Non-Abelian String Junctions as Confined Monopoles","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"A. Yung, M. Shifman","submitted_at":"2004-03-14T17:21:28Z","abstract_excerpt":"Various dynamical regimes associated with confined monopoles in the Higgs phase of N=2 two-flavor QCD are studied. The microscopic model we deal with has the SU(2)xU(1) gauge group, with a Fayet-Iliopoulos term of the U(1) factor, and large and (nearly) degenerate mass terms of the matter hypermultiplets. We present a complete quasiclassical treatment of the BPS sector of this model, including the full set of the first-order equations, derivations of all relevant zero modes, and derivation of an effective low-energy theory for the corresponding collective coordinates. The macroscopic descripti"},"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/0403149","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-03-14T17:21:28Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"8566cc0e61eea627b03b6f0d69b9ff9da631e3cd1dfaa432988d8b455fcc9e5e","abstract_canon_sha256":"763f52634f002f7a8a59874afbc499a024cd54da96a42782c9c77cd12e426117"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:29:26.861074Z","signature_b64":"//hmE8LOmqQjApskTV4MaH9gZa6yWKqYGKsEPK3H8VIXo2rknR7Au2j7yDoaUKPFpfRHYAaRFEOu7GfaztaCDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e6ed2cbc1f4984be8b88b84ac2bd6b5b8326d93e6120aed44748174b3010de4","last_reissued_at":"2026-07-04T17:29:26.860509Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:29:26.860509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Abelian String Junctions as Confined Monopoles","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"A. Yung, M. Shifman","submitted_at":"2004-03-14T17:21:28Z","abstract_excerpt":"Various dynamical regimes associated with confined monopoles in the Higgs phase of N=2 two-flavor QCD are studied. The microscopic model we deal with has the SU(2)xU(1) gauge group, with a Fayet-Iliopoulos term of the U(1) factor, and large and (nearly) degenerate mass terms of the matter hypermultiplets. We present a complete quasiclassical treatment of the BPS sector of this model, including the full set of the first-order equations, derivations of all relevant zero modes, and derivation of an effective low-energy theory for the corresponding collective coordinates. The macroscopic descripti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0403149","kind":"arxiv","version":4},"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/0403149/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/0403149","created_at":"2026-07-04T17:29:26.860565+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0403149v4","created_at":"2026-07-04T17:29:26.860565+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0403149","created_at":"2026-07-04T17:29:26.860565+00:00"},{"alias_kind":"pith_short_12","alias_value":"RZXNFS6B6SME","created_at":"2026-07-04T17:29:26.860565+00:00"},{"alias_kind":"pith_short_16","alias_value":"RZXNFS6B6SMEX2FY","created_at":"2026-07-04T17:29:26.860565+00:00"},{"alias_kind":"pith_short_8","alias_value":"RZXNFS6B","created_at":"2026-07-04T17:29:26.860565+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.06550","citing_title":"Hadrons in $\\mathcal{N}=2$ supersymmetric QCD from non-Abelian string on 2D black hole","ref_index":3,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RZXNFS6B6SMEX2FYROCKYK6WWW","json":"https://pith.science/pith/RZXNFS6B6SMEX2FYROCKYK6WWW.json","graph_json":"https://pith.science/api/pith-number/RZXNFS6B6SMEX2FYROCKYK6WWW/graph.json","events_json":"https://pith.science/api/pith-number/RZXNFS6B6SMEX2FYROCKYK6WWW/events.json","paper":"https://pith.science/paper/RZXNFS6B"},"agent_actions":{"view_html":"https://pith.science/pith/RZXNFS6B6SMEX2FYROCKYK6WWW","download_json":"https://pith.science/pith/RZXNFS6B6SMEX2FYROCKYK6WWW.json","view_paper":"https://pith.science/paper/RZXNFS6B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0403149&json=true","fetch_graph":"https://pith.science/api/pith-number/RZXNFS6B6SMEX2FYROCKYK6WWW/graph.json","fetch_events":"https://pith.science/api/pith-number/RZXNFS6B6SMEX2FYROCKYK6WWW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RZXNFS6B6SMEX2FYROCKYK6WWW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RZXNFS6B6SMEX2FYROCKYK6WWW/action/storage_attestation","attest_author":"https://pith.science/pith/RZXNFS6B6SMEX2FYROCKYK6WWW/action/author_attestation","sign_citation":"https://pith.science/pith/RZXNFS6B6SMEX2FYROCKYK6WWW/action/citation_signature","submit_replication":"https://pith.science/pith/RZXNFS6B6SMEX2FYROCKYK6WWW/action/replication_record"}},"created_at":"2026-07-04T17:29:26.860565+00:00","updated_at":"2026-07-04T17:29:26.860565+00:00"}