{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:WSHPZ7BUZDFL6DMQB5M4PGLGO2","short_pith_number":"pith:WSHPZ7BU","schema_version":"1.0","canonical_sha256":"b48efcfc34c8cabf0d900f59c7996676bb61ba82aae08908c0c84b345940a1c9","source":{"kind":"arxiv","id":"1412.4654","version":1},"attestation_state":"computed","paper":{"title":"Electrically charged finite energy solutions of an $SO(5)$ and an $SU(3)$ Higgs-Chern-Simons--Yang-Mills-Higgs systems in $3+1$ dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"D. H. Tchrakian, Francisco Navarro-Lerida","submitted_at":"2014-12-15T16:09:48Z","abstract_excerpt":"We study spherically symmetric finite energy solutions of two Higgs-Chern-Simons--Yang-Mills-Higgs (HCS-YMH) models in $3+1$ dimensions, one with gauge group $SO(5)$ and the other with $SU(3)$. The Chern-Simons (CS) densities are defined in terms of both the Yang-Mills (YM) and Higgs fields and the choice of the two gauge groups is made so they do not vanish. The solutions of the $SO(5)$ model carry only electric charge and zero magnetic charge, while the solutions of the $SU(3)$ model are dyons carrying both electric and magnetic charges like the Julia-Zee (JZ) dyon. Unlike the latter however"},"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":"1412.4654","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-15T16:09:48Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"d7b3e3a568cada46368920cfd52732c377bb410a8175fdd7b93b052591562584","abstract_canon_sha256":"b0db5e00bca5af8169fc761ca379d4f784b495e0faf307d7d08b2900fea1c884"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:31:21.363563Z","signature_b64":"xjTgcVhAIQAbwFI1H/R0T/KjrM9cmayBhgaYG3aMxni1eEhpN2rf7xI8Hi5xqEvk6aZFU7B9/OkNCkQ41NadAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b48efcfc34c8cabf0d900f59c7996676bb61ba82aae08908c0c84b345940a1c9","last_reissued_at":"2026-05-18T01:31:21.363100Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:31:21.363100Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electrically charged finite energy solutions of an $SO(5)$ and an $SU(3)$ Higgs-Chern-Simons--Yang-Mills-Higgs systems in $3+1$ dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"D. H. Tchrakian, Francisco Navarro-Lerida","submitted_at":"2014-12-15T16:09:48Z","abstract_excerpt":"We study spherically symmetric finite energy solutions of two Higgs-Chern-Simons--Yang-Mills-Higgs (HCS-YMH) models in $3+1$ dimensions, one with gauge group $SO(5)$ and the other with $SU(3)$. The Chern-Simons (CS) densities are defined in terms of both the Yang-Mills (YM) and Higgs fields and the choice of the two gauge groups is made so they do not vanish. The solutions of the $SO(5)$ model carry only electric charge and zero magnetic charge, while the solutions of the $SU(3)$ model are dyons carrying both electric and magnetic charges like the Julia-Zee (JZ) dyon. Unlike the latter however"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.4654","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":""},"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":"1412.4654","created_at":"2026-05-18T01:31:21.363169+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.4654v1","created_at":"2026-05-18T01:31:21.363169+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.4654","created_at":"2026-05-18T01:31:21.363169+00:00"},{"alias_kind":"pith_short_12","alias_value":"WSHPZ7BUZDFL","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"WSHPZ7BUZDFL6DMQ","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"WSHPZ7BU","created_at":"2026-05-18T12:28:54.890064+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/WSHPZ7BUZDFL6DMQB5M4PGLGO2","json":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2.json","graph_json":"https://pith.science/api/pith-number/WSHPZ7BUZDFL6DMQB5M4PGLGO2/graph.json","events_json":"https://pith.science/api/pith-number/WSHPZ7BUZDFL6DMQB5M4PGLGO2/events.json","paper":"https://pith.science/paper/WSHPZ7BU"},"agent_actions":{"view_html":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2","download_json":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2.json","view_paper":"https://pith.science/paper/WSHPZ7BU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.4654&json=true","fetch_graph":"https://pith.science/api/pith-number/WSHPZ7BUZDFL6DMQB5M4PGLGO2/graph.json","fetch_events":"https://pith.science/api/pith-number/WSHPZ7BUZDFL6DMQB5M4PGLGO2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/action/storage_attestation","attest_author":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/action/author_attestation","sign_citation":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/action/citation_signature","submit_replication":"https://pith.science/pith/WSHPZ7BUZDFL6DMQB5M4PGLGO2/action/replication_record"}},"created_at":"2026-05-18T01:31:21.363169+00:00","updated_at":"2026-05-18T01:31:21.363169+00:00"}