{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:SJEX53PVCO7EC3IJUCDPBOKSZT","short_pith_number":"pith:SJEX53PV","schema_version":"1.0","canonical_sha256":"92497eedf513be416d09a086f0b952cceb2429dd63072f4dcdc8681f06811b9e","source":{"kind":"arxiv","id":"1112.1492","version":4},"attestation_state":"computed","paper":{"title":"Particles of One-Half Topological Charge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ban-Loong Ng, Khai-Ming Wong, Rosy Teh","submitted_at":"2011-12-07T07:54:34Z","abstract_excerpt":"We would like to show the existence of finite energy SU(2) Yang-Mills-Higgs particles of one-half topological charge. The magnetic fields of these solutions at spatial infinity correspond to the magnetic field of a positive one-half magnetic monopole located at the origin and a semi-infinite Dirac string which carries a magnetic flux of $\\frac{2\\pi}{g}$ going into the center of the sphere at infinity. Hence the net magnetic charge of the configuration is zero. The solutions possess gauge potentials that are singular along one-half of the z-axis, elsewhere they are regular. There are two distin"},"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":"1112.1492","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-07T07:54:34Z","cross_cats_sorted":[],"title_canon_sha256":"57e3d3b159a00fc1e2f535325e5e9da8a40f96530cc11b7de1d8290021f9d4bb","abstract_canon_sha256":"f9d1a74aeb3f2bb9a6bebaf1829a27dc40269e87f50208d3240c74b5dc3bdbd3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:49:19.849277Z","signature_b64":"B9UlkSgvnTQqASJ9+eBf9mLFWvBO7rxSxwzJaWHyrUQYCL2/iSzu/9AEtDtaVPcDywrfwEaxKJwcFrihbqWuCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"92497eedf513be416d09a086f0b952cceb2429dd63072f4dcdc8681f06811b9e","last_reissued_at":"2026-05-18T03:49:19.848584Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:49:19.848584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Particles of One-Half Topological Charge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ban-Loong Ng, Khai-Ming Wong, Rosy Teh","submitted_at":"2011-12-07T07:54:34Z","abstract_excerpt":"We would like to show the existence of finite energy SU(2) Yang-Mills-Higgs particles of one-half topological charge. The magnetic fields of these solutions at spatial infinity correspond to the magnetic field of a positive one-half magnetic monopole located at the origin and a semi-infinite Dirac string which carries a magnetic flux of $\\frac{2\\pi}{g}$ going into the center of the sphere at infinity. Hence the net magnetic charge of the configuration is zero. The solutions possess gauge potentials that are singular along one-half of the z-axis, elsewhere they are regular. There are two distin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.1492","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":""},"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":"1112.1492","created_at":"2026-05-18T03:49:19.848690+00:00"},{"alias_kind":"arxiv_version","alias_value":"1112.1492v4","created_at":"2026-05-18T03:49:19.848690+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.1492","created_at":"2026-05-18T03:49:19.848690+00:00"},{"alias_kind":"pith_short_12","alias_value":"SJEX53PVCO7E","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_16","alias_value":"SJEX53PVCO7EC3IJ","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_8","alias_value":"SJEX53PV","created_at":"2026-05-18T12:26:41.206345+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SJEX53PVCO7EC3IJUCDPBOKSZT","json":"https://pith.science/pith/SJEX53PVCO7EC3IJUCDPBOKSZT.json","graph_json":"https://pith.science/api/pith-number/SJEX53PVCO7EC3IJUCDPBOKSZT/graph.json","events_json":"https://pith.science/api/pith-number/SJEX53PVCO7EC3IJUCDPBOKSZT/events.json","paper":"https://pith.science/paper/SJEX53PV"},"agent_actions":{"view_html":"https://pith.science/pith/SJEX53PVCO7EC3IJUCDPBOKSZT","download_json":"https://pith.science/pith/SJEX53PVCO7EC3IJUCDPBOKSZT.json","view_paper":"https://pith.science/paper/SJEX53PV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1112.1492&json=true","fetch_graph":"https://pith.science/api/pith-number/SJEX53PVCO7EC3IJUCDPBOKSZT/graph.json","fetch_events":"https://pith.science/api/pith-number/SJEX53PVCO7EC3IJUCDPBOKSZT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SJEX53PVCO7EC3IJUCDPBOKSZT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SJEX53PVCO7EC3IJUCDPBOKSZT/action/storage_attestation","attest_author":"https://pith.science/pith/SJEX53PVCO7EC3IJUCDPBOKSZT/action/author_attestation","sign_citation":"https://pith.science/pith/SJEX53PVCO7EC3IJUCDPBOKSZT/action/citation_signature","submit_replication":"https://pith.science/pith/SJEX53PVCO7EC3IJUCDPBOKSZT/action/replication_record"}},"created_at":"2026-05-18T03:49:19.848690+00:00","updated_at":"2026-05-18T03:49:19.848690+00:00"}