{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:GKT44HAKTL22AAI5ULJW4FIECM","short_pith_number":"pith:GKT44HAK","schema_version":"1.0","canonical_sha256":"32a7ce1c0a9af5a0011da2d36e1504130e7423e68a88eb0de9a5b5264427d751","source":{"kind":"arxiv","id":"hep-th/9310094","version":3},"attestation_state":"computed","paper":{"title":"Composite gauge field models with broken symmetries","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"B. S. Balakrishna, K. T. Mahanthappa","submitted_at":"1993-10-15T14:07:47Z","abstract_excerpt":"We present a generalization of the non-Abelian version of the $CP^{N-1}$ models (also known as Grassmannian models) that involve composite gauge fields to accommodate partial breaking of the non-Abelian gauge symmetry. For this to be possible, in most cases, the constituent fields need to belong to an anomaly free complex representation. Symmetry is broken dynamically for large $N$ primarily by a naturally generated composite scalar which simulates Higgs mechanism. In the example studied in some detail, the gauge group SO(10) gets broken down to subgroups like SU(5) or SU(5)$\\times$U(1)."},"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/9310094","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1993-10-15T14:07:47Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"2a68bb2152065bf89ace363e3f83523ff11ba020ca4981b0c71afc18b8038356","abstract_canon_sha256":"9f1007a2556e42204d3d2b55c3de21c5ca4e429065941680acb9e7e5d7dcc162"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:18:55.391936Z","signature_b64":"ICOyErGCFaL3AtnLHtRj/4yOdWpJ4ldv1QdCikF7bDpb34yN4pBRUmBVNEowCnjC+/QaTkRnh0K3fNudkUgoCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"32a7ce1c0a9af5a0011da2d36e1504130e7423e68a88eb0de9a5b5264427d751","last_reissued_at":"2026-07-04T17:18:55.391591Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:18:55.391591Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Composite gauge field models with broken symmetries","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"B. S. Balakrishna, K. T. Mahanthappa","submitted_at":"1993-10-15T14:07:47Z","abstract_excerpt":"We present a generalization of the non-Abelian version of the $CP^{N-1}$ models (also known as Grassmannian models) that involve composite gauge fields to accommodate partial breaking of the non-Abelian gauge symmetry. For this to be possible, in most cases, the constituent fields need to belong to an anomaly free complex representation. Symmetry is broken dynamically for large $N$ primarily by a naturally generated composite scalar which simulates Higgs mechanism. In the example studied in some detail, the gauge group SO(10) gets broken down to subgroups like SU(5) or SU(5)$\\times$U(1)."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9310094","kind":"arxiv","version":3},"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/9310094/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/9310094","created_at":"2026-07-04T17:18:55.391648+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9310094v3","created_at":"2026-07-04T17:18:55.391648+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9310094","created_at":"2026-07-04T17:18:55.391648+00:00"},{"alias_kind":"pith_short_12","alias_value":"GKT44HAKTL22","created_at":"2026-07-04T17:18:55.391648+00:00"},{"alias_kind":"pith_short_16","alias_value":"GKT44HAKTL22AAI5","created_at":"2026-07-04T17:18:55.391648+00:00"},{"alias_kind":"pith_short_8","alias_value":"GKT44HAK","created_at":"2026-07-04T17:18:55.391648+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/GKT44HAKTL22AAI5ULJW4FIECM","json":"https://pith.science/pith/GKT44HAKTL22AAI5ULJW4FIECM.json","graph_json":"https://pith.science/api/pith-number/GKT44HAKTL22AAI5ULJW4FIECM/graph.json","events_json":"https://pith.science/api/pith-number/GKT44HAKTL22AAI5ULJW4FIECM/events.json","paper":"https://pith.science/paper/GKT44HAK"},"agent_actions":{"view_html":"https://pith.science/pith/GKT44HAKTL22AAI5ULJW4FIECM","download_json":"https://pith.science/pith/GKT44HAKTL22AAI5ULJW4FIECM.json","view_paper":"https://pith.science/paper/GKT44HAK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9310094&json=true","fetch_graph":"https://pith.science/api/pith-number/GKT44HAKTL22AAI5ULJW4FIECM/graph.json","fetch_events":"https://pith.science/api/pith-number/GKT44HAKTL22AAI5ULJW4FIECM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GKT44HAKTL22AAI5ULJW4FIECM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GKT44HAKTL22AAI5ULJW4FIECM/action/storage_attestation","attest_author":"https://pith.science/pith/GKT44HAKTL22AAI5ULJW4FIECM/action/author_attestation","sign_citation":"https://pith.science/pith/GKT44HAKTL22AAI5ULJW4FIECM/action/citation_signature","submit_replication":"https://pith.science/pith/GKT44HAKTL22AAI5ULJW4FIECM/action/replication_record"}},"created_at":"2026-07-04T17:18:55.391648+00:00","updated_at":"2026-07-04T17:18:55.391648+00:00"}