{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:5T5JBTLEBMFVZY4PP2KEOBQFKL","short_pith_number":"pith:5T5JBTLE","schema_version":"1.0","canonical_sha256":"ecfa90cd640b0b5ce38f7e9447060552c8948bf9265dbf9c8af77cb281546bab","source":{"kind":"arxiv","id":"hep-th/9502059","version":1},"attestation_state":"computed","paper":{"title":"Canonical quantization of spontaneously broken topologically massive gauge theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Edwin Lim-Lombridas (University of Connecticut), Gerald Dunne, Kurt Haller, Lusheng Chen","submitted_at":"1995-02-09T20:05:40Z","abstract_excerpt":"In this paper we investigate the canonical quantization of a non-Abelian topologically massive Chern-Simons theory in which the gauge fields are minimally coupled to a multiplet of scalar fields in such a way that the gauge symmetry is spontaneously broken. Such a model produces the Chern-Simons-Higgs mechanism in which the gauge excitations acquire mass both from the Chern-Simons term and from the Higgs-Kibble effect. The symmetry breaking is chosen to be only partially broken, in such a way that in the broken vacuum there remains a residual non-Abelian symmetry. We develop the canonical oper"},"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/9502059","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1995-02-09T20:05:40Z","cross_cats_sorted":[],"title_canon_sha256":"b09e9d91546f0fb0f1a0cfc137164402606cc88dd48d836c63ab2dcc4fd47c7d","abstract_canon_sha256":"eebccbc433f2223795bd3e7263fdbcccff23052a1883ca582567ff0af767777f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:03.280245Z","signature_b64":"RFO2mGyxlnKy2Lm+wCOETiztQ4FxkmJrCLAPzYhcmXnKsKdbiR1JtIe3wSoKHrZBkE5olFUwmW2I5IlJ3k5XDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ecfa90cd640b0b5ce38f7e9447060552c8948bf9265dbf9c8af77cb281546bab","last_reissued_at":"2026-05-18T01:06:03.279747Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:03.279747Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Canonical quantization of spontaneously broken topologically massive gauge theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Edwin Lim-Lombridas (University of Connecticut), Gerald Dunne, Kurt Haller, Lusheng Chen","submitted_at":"1995-02-09T20:05:40Z","abstract_excerpt":"In this paper we investigate the canonical quantization of a non-Abelian topologically massive Chern-Simons theory in which the gauge fields are minimally coupled to a multiplet of scalar fields in such a way that the gauge symmetry is spontaneously broken. Such a model produces the Chern-Simons-Higgs mechanism in which the gauge excitations acquire mass both from the Chern-Simons term and from the Higgs-Kibble effect. The symmetry breaking is chosen to be only partially broken, in such a way that in the broken vacuum there remains a residual non-Abelian symmetry. We develop the canonical oper"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9502059","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/9502059","created_at":"2026-05-18T01:06:03.279827+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9502059v1","created_at":"2026-05-18T01:06:03.279827+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9502059","created_at":"2026-05-18T01:06:03.279827+00:00"},{"alias_kind":"pith_short_12","alias_value":"5T5JBTLEBMFV","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"5T5JBTLEBMFVZY4P","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"5T5JBTLE","created_at":"2026-05-18T12:25:47.102015+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/5T5JBTLEBMFVZY4PP2KEOBQFKL","json":"https://pith.science/pith/5T5JBTLEBMFVZY4PP2KEOBQFKL.json","graph_json":"https://pith.science/api/pith-number/5T5JBTLEBMFVZY4PP2KEOBQFKL/graph.json","events_json":"https://pith.science/api/pith-number/5T5JBTLEBMFVZY4PP2KEOBQFKL/events.json","paper":"https://pith.science/paper/5T5JBTLE"},"agent_actions":{"view_html":"https://pith.science/pith/5T5JBTLEBMFVZY4PP2KEOBQFKL","download_json":"https://pith.science/pith/5T5JBTLEBMFVZY4PP2KEOBQFKL.json","view_paper":"https://pith.science/paper/5T5JBTLE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9502059&json=true","fetch_graph":"https://pith.science/api/pith-number/5T5JBTLEBMFVZY4PP2KEOBQFKL/graph.json","fetch_events":"https://pith.science/api/pith-number/5T5JBTLEBMFVZY4PP2KEOBQFKL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5T5JBTLEBMFVZY4PP2KEOBQFKL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5T5JBTLEBMFVZY4PP2KEOBQFKL/action/storage_attestation","attest_author":"https://pith.science/pith/5T5JBTLEBMFVZY4PP2KEOBQFKL/action/author_attestation","sign_citation":"https://pith.science/pith/5T5JBTLEBMFVZY4PP2KEOBQFKL/action/citation_signature","submit_replication":"https://pith.science/pith/5T5JBTLEBMFVZY4PP2KEOBQFKL/action/replication_record"}},"created_at":"2026-05-18T01:06:03.279827+00:00","updated_at":"2026-05-18T01:06:03.279827+00:00"}