{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:DKMKAYGE4MIGFCBTAQLKQYU24P","short_pith_number":"pith:DKMKAYGE","schema_version":"1.0","canonical_sha256":"1a98a060c4e3106288330416a8629ae3d2ed0304cfc2bee77a9033b31a1f0e63","source":{"kind":"arxiv","id":"hep-th/9503096","version":1},"attestation_state":"computed","paper":{"title":"Composite Gauge fields and Broken Symmetries","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. S. Balakrishna, K. T. Mahanthappa","submitted_at":"1995-03-14T17:14:46Z","abstract_excerpt":"A generalization of the non-Abelian version of the $CP^{N-1}$ models (also known as Grassmannian models) is presented. The generalization helps accommodate a partial breaking of the non-Abelian gauge symmetry. Constituents of the composite gauge fields, in many cases, are naturally constrained to belong to an anomaly free representation which in turn generates a composite scalar simulating Higgs mechanism to break the gauge symmetry dynamically for large $N$. Two cases are studied in detail: one based on the SU(2) gauge group and the other on SO(10). Breakings such as SU(2)$\\to$U(1) or SO(10)$"},"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/9503096","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1995-03-14T17:14:46Z","cross_cats_sorted":[],"title_canon_sha256":"dda9afc8352225ca3ea46c93180a3606b701c797d5428b0295eafcf52eed8146","abstract_canon_sha256":"ffbec9c610b294a4f26e3499c06835f8553334873d5866ee45fd469882afdf22"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:01.310091Z","signature_b64":"/zb0M/n4dlDT5oHOK4ER7iXJ/egaL+zc0ryX5fr9CZ9BI+ePdiS8XKKSmZL5HKfhJQcU4fHj5udHlaYJnrL7Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1a98a060c4e3106288330416a8629ae3d2ed0304cfc2bee77a9033b31a1f0e63","last_reissued_at":"2026-05-18T01:06:01.309699Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:01.309699Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Composite Gauge fields and Broken Symmetries","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. S. Balakrishna, K. T. Mahanthappa","submitted_at":"1995-03-14T17:14:46Z","abstract_excerpt":"A generalization of the non-Abelian version of the $CP^{N-1}$ models (also known as Grassmannian models) is presented. The generalization helps accommodate a partial breaking of the non-Abelian gauge symmetry. Constituents of the composite gauge fields, in many cases, are naturally constrained to belong to an anomaly free representation which in turn generates a composite scalar simulating Higgs mechanism to break the gauge symmetry dynamically for large $N$. Two cases are studied in detail: one based on the SU(2) gauge group and the other on SO(10). Breakings such as SU(2)$\\to$U(1) or SO(10)$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9503096","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":"hep-th/9503096","created_at":"2026-05-18T01:06:01.309757+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9503096v1","created_at":"2026-05-18T01:06:01.309757+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9503096","created_at":"2026-05-18T01:06:01.309757+00:00"},{"alias_kind":"pith_short_12","alias_value":"DKMKAYGE4MIG","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"DKMKAYGE4MIGFCBT","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"DKMKAYGE","created_at":"2026-05-18T12:25:47.700082+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/DKMKAYGE4MIGFCBTAQLKQYU24P","json":"https://pith.science/pith/DKMKAYGE4MIGFCBTAQLKQYU24P.json","graph_json":"https://pith.science/api/pith-number/DKMKAYGE4MIGFCBTAQLKQYU24P/graph.json","events_json":"https://pith.science/api/pith-number/DKMKAYGE4MIGFCBTAQLKQYU24P/events.json","paper":"https://pith.science/paper/DKMKAYGE"},"agent_actions":{"view_html":"https://pith.science/pith/DKMKAYGE4MIGFCBTAQLKQYU24P","download_json":"https://pith.science/pith/DKMKAYGE4MIGFCBTAQLKQYU24P.json","view_paper":"https://pith.science/paper/DKMKAYGE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9503096&json=true","fetch_graph":"https://pith.science/api/pith-number/DKMKAYGE4MIGFCBTAQLKQYU24P/graph.json","fetch_events":"https://pith.science/api/pith-number/DKMKAYGE4MIGFCBTAQLKQYU24P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DKMKAYGE4MIGFCBTAQLKQYU24P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DKMKAYGE4MIGFCBTAQLKQYU24P/action/storage_attestation","attest_author":"https://pith.science/pith/DKMKAYGE4MIGFCBTAQLKQYU24P/action/author_attestation","sign_citation":"https://pith.science/pith/DKMKAYGE4MIGFCBTAQLKQYU24P/action/citation_signature","submit_replication":"https://pith.science/pith/DKMKAYGE4MIGFCBTAQLKQYU24P/action/replication_record"}},"created_at":"2026-05-18T01:06:01.309757+00:00","updated_at":"2026-05-18T01:06:01.309757+00:00"}