{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:DNI7FM2RPTLM5N22BJUKKHZ3ZZ","short_pith_number":"pith:DNI7FM2R","schema_version":"1.0","canonical_sha256":"1b51f2b3517cd6ceb75a0a68a51f3bce580ae9b9f37f7f4bbbf4e0e7599fb926","source":{"kind":"arxiv","id":"1012.4057","version":2},"attestation_state":"computed","paper":{"title":"Non-Abelian Monopoles in the Higgs Phase","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Muneto Nitta, Walter Vinci","submitted_at":"2010-12-18T04:15:51Z","abstract_excerpt":"We use the moduli matrix approach to study the moduli space of 1/4 BPS kinks supported by vortices in the Higgs phase of N = 2 supersymmetric U(N) gauge theories when non-zero masses for the matter hypermultiplets are introduced. We focus on the case of degenerate masses. In these special cases vortices acquire new orientational degrees of freedom, and become \"non-Abelian\". Kinks acquire new degrees of freedom too, and we will refer to them as \"non-Abelian\". As already noticed for the Abelian case, non-Abelian kinks must correspond to non-Abelian monopoles of the unbroken phase of SU(N) Yang-M"},"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":"1012.4057","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-12-18T04:15:51Z","cross_cats_sorted":["hep-ph","math-ph","math.MP"],"title_canon_sha256":"0410d9e5b01234f8b0cea64bbf5cc7fae0e326b9f58faae5076bd30608ca1f97","abstract_canon_sha256":"d97ab1eaf1e816fada8d19b32c48292af117970850a8b56708d7033da0466533"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:25:37.643101Z","signature_b64":"xEFVxBRJSOoM6yRwmEkXQ1v98BYUw0nV+9XVix6WjsWCC64izzRCybdUYK5u7RAk4Kvuk1asS3oVpbsydbVmDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1b51f2b3517cd6ceb75a0a68a51f3bce580ae9b9f37f7f4bbbf4e0e7599fb926","last_reissued_at":"2026-05-18T04:25:37.642622Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:25:37.642622Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Abelian Monopoles in the Higgs Phase","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Muneto Nitta, Walter Vinci","submitted_at":"2010-12-18T04:15:51Z","abstract_excerpt":"We use the moduli matrix approach to study the moduli space of 1/4 BPS kinks supported by vortices in the Higgs phase of N = 2 supersymmetric U(N) gauge theories when non-zero masses for the matter hypermultiplets are introduced. We focus on the case of degenerate masses. In these special cases vortices acquire new orientational degrees of freedom, and become \"non-Abelian\". Kinks acquire new degrees of freedom too, and we will refer to them as \"non-Abelian\". As already noticed for the Abelian case, non-Abelian kinks must correspond to non-Abelian monopoles of the unbroken phase of SU(N) Yang-M"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1012.4057","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":""},"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":"1012.4057","created_at":"2026-05-18T04:25:37.642694+00:00"},{"alias_kind":"arxiv_version","alias_value":"1012.4057v2","created_at":"2026-05-18T04:25:37.642694+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1012.4057","created_at":"2026-05-18T04:25:37.642694+00:00"},{"alias_kind":"pith_short_12","alias_value":"DNI7FM2RPTLM","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_16","alias_value":"DNI7FM2RPTLM5N22","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_8","alias_value":"DNI7FM2R","created_at":"2026-05-18T12:26:06.534383+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.12802","citing_title":"Fractional instantons in 2d $\\mathbb{C}P^{N-1}$ model and 4d Yang-Mills theory with 't Hooft twists","ref_index":72,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DNI7FM2RPTLM5N22BJUKKHZ3ZZ","json":"https://pith.science/pith/DNI7FM2RPTLM5N22BJUKKHZ3ZZ.json","graph_json":"https://pith.science/api/pith-number/DNI7FM2RPTLM5N22BJUKKHZ3ZZ/graph.json","events_json":"https://pith.science/api/pith-number/DNI7FM2RPTLM5N22BJUKKHZ3ZZ/events.json","paper":"https://pith.science/paper/DNI7FM2R"},"agent_actions":{"view_html":"https://pith.science/pith/DNI7FM2RPTLM5N22BJUKKHZ3ZZ","download_json":"https://pith.science/pith/DNI7FM2RPTLM5N22BJUKKHZ3ZZ.json","view_paper":"https://pith.science/paper/DNI7FM2R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1012.4057&json=true","fetch_graph":"https://pith.science/api/pith-number/DNI7FM2RPTLM5N22BJUKKHZ3ZZ/graph.json","fetch_events":"https://pith.science/api/pith-number/DNI7FM2RPTLM5N22BJUKKHZ3ZZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DNI7FM2RPTLM5N22BJUKKHZ3ZZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DNI7FM2RPTLM5N22BJUKKHZ3ZZ/action/storage_attestation","attest_author":"https://pith.science/pith/DNI7FM2RPTLM5N22BJUKKHZ3ZZ/action/author_attestation","sign_citation":"https://pith.science/pith/DNI7FM2RPTLM5N22BJUKKHZ3ZZ/action/citation_signature","submit_replication":"https://pith.science/pith/DNI7FM2RPTLM5N22BJUKKHZ3ZZ/action/replication_record"}},"created_at":"2026-05-18T04:25:37.642694+00:00","updated_at":"2026-05-18T04:25:37.642694+00:00"}