{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:VBMJIE7KZ5GZC4CT7QKNVX2PEO","short_pith_number":"pith:VBMJIE7K","schema_version":"1.0","canonical_sha256":"a8589413eacf4d917053fc14dadf4f238bc0bca5d517404efa775ec10b6a1cfb","source":{"kind":"arxiv","id":"hep-th/9601028","version":1},"attestation_state":"computed","paper":{"title":"Monopoles in Weinberg-Salam Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. Maison, Y. M. Cho","submitted_at":"1996-01-09T05:31:59Z","abstract_excerpt":"We present a new type of spherically symmetric monopole and dyon solutions with the magnetic charge $ 4\\pi/e$ in the standard Weinberg-Salam model. The monopole (and dyon) could be interpreted as a non-trivial hybrid between the abelian Dirac monopole and non-abelian 't Hooft-Polyakov monopole (with an electric charge). We discuss the possible physical implications of the electroweak dyon."},"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/9601028","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-01-09T05:31:59Z","cross_cats_sorted":[],"title_canon_sha256":"531c28c6c6aa89b0a9162204436745d78fca4f25fd042cb6fc84fbd0ae08462a","abstract_canon_sha256":"d4df2b1301e57dba220edad7be4fd90ce572379710ccf5b9410011b5a1dfadd3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:02:02.294704Z","signature_b64":"cJS6Ygmb01vsvnYAqaVnnvUpwnL4RQE0hyM9IavDWQ0VUAaGh5syrWwDwM1u5CnuFoeVss+OWDh2c5T2JwcuBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a8589413eacf4d917053fc14dadf4f238bc0bca5d517404efa775ec10b6a1cfb","last_reissued_at":"2026-07-04T16:02:02.294301Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:02:02.294301Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Monopoles in Weinberg-Salam Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. Maison, Y. M. Cho","submitted_at":"1996-01-09T05:31:59Z","abstract_excerpt":"We present a new type of spherically symmetric monopole and dyon solutions with the magnetic charge $ 4\\pi/e$ in the standard Weinberg-Salam model. The monopole (and dyon) could be interpreted as a non-trivial hybrid between the abelian Dirac monopole and non-abelian 't Hooft-Polyakov monopole (with an electric charge). We discuss the possible physical implications of the electroweak dyon."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9601028","kind":"arxiv","version":1},"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/9601028/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/9601028","created_at":"2026-07-04T16:02:02.294370+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9601028v1","created_at":"2026-07-04T16:02:02.294370+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9601028","created_at":"2026-07-04T16:02:02.294370+00:00"},{"alias_kind":"pith_short_12","alias_value":"VBMJIE7KZ5GZ","created_at":"2026-07-04T16:02:02.294370+00:00"},{"alias_kind":"pith_short_16","alias_value":"VBMJIE7KZ5GZC4CT","created_at":"2026-07-04T16:02:02.294370+00:00"},{"alias_kind":"pith_short_8","alias_value":"VBMJIE7K","created_at":"2026-07-04T16:02:02.294370+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.08603","citing_title":"Self-Gravitating Magnetic Monopoles and Dyons in String-Inspired Models: Structure and Stability","ref_index":24,"is_internal_anchor":true},{"citing_arxiv_id":"2312.01355","citing_title":"The electroweak magnetic monopole in the presence of KSVZ axion","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"2605.02869","citing_title":"Magnetic Monopoles -- From Dirac to the Large Hadron Collider","ref_index":10,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07300","citing_title":"Constraining magnetic monopoles and multiply charged particles with diphoton events at the LHC","ref_index":78,"is_internal_anchor":false},{"citing_arxiv_id":"2605.07348","citing_title":"Generalizations and UV completions of Cho-Maison monopole","ref_index":1,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VBMJIE7KZ5GZC4CT7QKNVX2PEO","json":"https://pith.science/pith/VBMJIE7KZ5GZC4CT7QKNVX2PEO.json","graph_json":"https://pith.science/api/pith-number/VBMJIE7KZ5GZC4CT7QKNVX2PEO/graph.json","events_json":"https://pith.science/api/pith-number/VBMJIE7KZ5GZC4CT7QKNVX2PEO/events.json","paper":"https://pith.science/paper/VBMJIE7K"},"agent_actions":{"view_html":"https://pith.science/pith/VBMJIE7KZ5GZC4CT7QKNVX2PEO","download_json":"https://pith.science/pith/VBMJIE7KZ5GZC4CT7QKNVX2PEO.json","view_paper":"https://pith.science/paper/VBMJIE7K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9601028&json=true","fetch_graph":"https://pith.science/api/pith-number/VBMJIE7KZ5GZC4CT7QKNVX2PEO/graph.json","fetch_events":"https://pith.science/api/pith-number/VBMJIE7KZ5GZC4CT7QKNVX2PEO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VBMJIE7KZ5GZC4CT7QKNVX2PEO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VBMJIE7KZ5GZC4CT7QKNVX2PEO/action/storage_attestation","attest_author":"https://pith.science/pith/VBMJIE7KZ5GZC4CT7QKNVX2PEO/action/author_attestation","sign_citation":"https://pith.science/pith/VBMJIE7KZ5GZC4CT7QKNVX2PEO/action/citation_signature","submit_replication":"https://pith.science/pith/VBMJIE7KZ5GZC4CT7QKNVX2PEO/action/replication_record"}},"created_at":"2026-07-04T16:02:02.294370+00:00","updated_at":"2026-07-04T16:02:02.294370+00:00"}