{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:R2R6XXCQ3PZJJA6UUAZXRW2EEV","short_pith_number":"pith:R2R6XXCQ","schema_version":"1.0","canonical_sha256":"8ea3ebdc50dbf29483d4a03378db4425622479119ceefc2dc40dc097b348eb85","source":{"kind":"arxiv","id":"1402.4222","version":8},"attestation_state":"computed","paper":{"title":"MAP, MAC, and Vortex-rings Configurations in the Weinberg-Salam Model","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":"2014-02-18T04:20:58Z","abstract_excerpt":"We report on the presence of new axially symmetric monopoles, antimonopoles and vortex-rings solutions of the SU(2)$\\times$U(1) Weinberg-Salam model of electromagnetic and weak interactions. When the $\\phi$-winding number $n=1$, and 2, the configurations are monopole-antimonopole pair (MAP) and monopole-antimonopole chain (MAC) with poles of alternating sign magnetic charge arranged along the $z$-axis. Vortex-rings start to appear from the MAP and MAC configurations when the winding number $n=3$. The MAP configurations possess zero net magnetic charge whereas the MAC configurations possess net"},"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":"1402.4222","kind":"arxiv","version":8},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-18T04:20:58Z","cross_cats_sorted":[],"title_canon_sha256":"a3cbef183d56f2c730bc2a0f6937c78b016022ea9c4a0aae3a76bccab42f284e","abstract_canon_sha256":"2fe17011cf39b8a1bbed3af3645bcc0eb9763501d47a06ec96f7e37d7b0f74c6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:20:49.863479Z","signature_b64":"W7p+Hg2JeNUOMQU7Bmr2ypzpp6WQTknlnJN7mMF8+OjfRDCkXUlQbzF2cfaQ88HXlCHHvY2JT3AHrzijv9CuCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8ea3ebdc50dbf29483d4a03378db4425622479119ceefc2dc40dc097b348eb85","last_reissued_at":"2026-05-18T02:20:49.862669Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:20:49.862669Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"MAP, MAC, and Vortex-rings Configurations in the Weinberg-Salam Model","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":"2014-02-18T04:20:58Z","abstract_excerpt":"We report on the presence of new axially symmetric monopoles, antimonopoles and vortex-rings solutions of the SU(2)$\\times$U(1) Weinberg-Salam model of electromagnetic and weak interactions. When the $\\phi$-winding number $n=1$, and 2, the configurations are monopole-antimonopole pair (MAP) and monopole-antimonopole chain (MAC) with poles of alternating sign magnetic charge arranged along the $z$-axis. Vortex-rings start to appear from the MAP and MAC configurations when the winding number $n=3$. The MAP configurations possess zero net magnetic charge whereas the MAC configurations possess net"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.4222","kind":"arxiv","version":8},"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":"1402.4222","created_at":"2026-05-18T02:20:49.862799+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.4222v8","created_at":"2026-05-18T02:20:49.862799+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.4222","created_at":"2026-05-18T02:20:49.862799+00:00"},{"alias_kind":"pith_short_12","alias_value":"R2R6XXCQ3PZJ","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_16","alias_value":"R2R6XXCQ3PZJJA6U","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_8","alias_value":"R2R6XXCQ","created_at":"2026-05-18T12:28:46.137349+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.05342","citing_title":"Bifurcations in Bosonic Stars: chains and rings from spherical solutions","ref_index":48,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/R2R6XXCQ3PZJJA6UUAZXRW2EEV","json":"https://pith.science/pith/R2R6XXCQ3PZJJA6UUAZXRW2EEV.json","graph_json":"https://pith.science/api/pith-number/R2R6XXCQ3PZJJA6UUAZXRW2EEV/graph.json","events_json":"https://pith.science/api/pith-number/R2R6XXCQ3PZJJA6UUAZXRW2EEV/events.json","paper":"https://pith.science/paper/R2R6XXCQ"},"agent_actions":{"view_html":"https://pith.science/pith/R2R6XXCQ3PZJJA6UUAZXRW2EEV","download_json":"https://pith.science/pith/R2R6XXCQ3PZJJA6UUAZXRW2EEV.json","view_paper":"https://pith.science/paper/R2R6XXCQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.4222&json=true","fetch_graph":"https://pith.science/api/pith-number/R2R6XXCQ3PZJJA6UUAZXRW2EEV/graph.json","fetch_events":"https://pith.science/api/pith-number/R2R6XXCQ3PZJJA6UUAZXRW2EEV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R2R6XXCQ3PZJJA6UUAZXRW2EEV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R2R6XXCQ3PZJJA6UUAZXRW2EEV/action/storage_attestation","attest_author":"https://pith.science/pith/R2R6XXCQ3PZJJA6UUAZXRW2EEV/action/author_attestation","sign_citation":"https://pith.science/pith/R2R6XXCQ3PZJJA6UUAZXRW2EEV/action/citation_signature","submit_replication":"https://pith.science/pith/R2R6XXCQ3PZJJA6UUAZXRW2EEV/action/replication_record"}},"created_at":"2026-05-18T02:20:49.862799+00:00","updated_at":"2026-05-18T02:20:49.862799+00:00"}