{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:SSUVTBIGNOKBZIGVCNUNBDSZNK","short_pith_number":"pith:SSUVTBIG","schema_version":"1.0","canonical_sha256":"94a95985066b941ca0d51368d08e596a9d97feb057d6f0a9dea0a88a095d82dd","source":{"kind":"arxiv","id":"1310.5582","version":2},"attestation_state":"computed","paper":{"title":"Antisymmetric tensor Z_p gauge symmetries in field theory and string theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Angel M. Uranga, Guillermo Ram\\'irez, Mikel Berasaluce-Gonz\\'alez","submitted_at":"2013-10-21T15:00:43Z","abstract_excerpt":"We consider discrete gauge symmetries in D dimensions arising as remnants of broken continuous gauge symmetries carried by general antisymmetric tensor fields, rather than by standard 1-forms. The lagrangian for such a general ${\\bf Z}_p$ gauge theory can be described in terms of a $r$-form gauge field made massive by a $(r-1)$-form, or other dual realizations, that we also discuss. The theory contains charged topological defects of different dimensionalities, generalizing the familiar charged particles and strings in D=4. We describe realizations in string theory compactifications with torsio"},"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":"1310.5582","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-10-21T15:00:43Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"036fdf601047e61d84da4ecaf8135d4afc58490f660b34cb2faa4a825030125a","abstract_canon_sha256":"8ddea7f76aee51e8a6db854101693b010848b17f8a89b26bfd402f2571c5315a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:46:56.912726Z","signature_b64":"3dGS0+BAfAMVUKewKn1IaUQQHmmDJv+V9S6VNmBIPfeHYfqUAWeapmly3Ho1PY+mrje5AhwUG2oaRFI80jACAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"94a95985066b941ca0d51368d08e596a9d97feb057d6f0a9dea0a88a095d82dd","last_reissued_at":"2026-05-18T01:46:56.912094Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:46:56.912094Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Antisymmetric tensor Z_p gauge symmetries in field theory and string theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Angel M. Uranga, Guillermo Ram\\'irez, Mikel Berasaluce-Gonz\\'alez","submitted_at":"2013-10-21T15:00:43Z","abstract_excerpt":"We consider discrete gauge symmetries in D dimensions arising as remnants of broken continuous gauge symmetries carried by general antisymmetric tensor fields, rather than by standard 1-forms. The lagrangian for such a general ${\\bf Z}_p$ gauge theory can be described in terms of a $r$-form gauge field made massive by a $(r-1)$-form, or other dual realizations, that we also discuss. The theory contains charged topological defects of different dimensionalities, generalizing the familiar charged particles and strings in D=4. We describe realizations in string theory compactifications with torsio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.5582","kind":"arxiv","version":2},"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":"1310.5582","created_at":"2026-05-18T01:46:56.912205+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.5582v2","created_at":"2026-05-18T01:46:56.912205+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.5582","created_at":"2026-05-18T01:46:56.912205+00:00"},{"alias_kind":"pith_short_12","alias_value":"SSUVTBIGNOKB","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_16","alias_value":"SSUVTBIGNOKBZIGV","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_8","alias_value":"SSUVTBIG","created_at":"2026-05-18T12:27:59.945178+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/SSUVTBIGNOKBZIGVCNUNBDSZNK","json":"https://pith.science/pith/SSUVTBIGNOKBZIGVCNUNBDSZNK.json","graph_json":"https://pith.science/api/pith-number/SSUVTBIGNOKBZIGVCNUNBDSZNK/graph.json","events_json":"https://pith.science/api/pith-number/SSUVTBIGNOKBZIGVCNUNBDSZNK/events.json","paper":"https://pith.science/paper/SSUVTBIG"},"agent_actions":{"view_html":"https://pith.science/pith/SSUVTBIGNOKBZIGVCNUNBDSZNK","download_json":"https://pith.science/pith/SSUVTBIGNOKBZIGVCNUNBDSZNK.json","view_paper":"https://pith.science/paper/SSUVTBIG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.5582&json=true","fetch_graph":"https://pith.science/api/pith-number/SSUVTBIGNOKBZIGVCNUNBDSZNK/graph.json","fetch_events":"https://pith.science/api/pith-number/SSUVTBIGNOKBZIGVCNUNBDSZNK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SSUVTBIGNOKBZIGVCNUNBDSZNK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SSUVTBIGNOKBZIGVCNUNBDSZNK/action/storage_attestation","attest_author":"https://pith.science/pith/SSUVTBIGNOKBZIGVCNUNBDSZNK/action/author_attestation","sign_citation":"https://pith.science/pith/SSUVTBIGNOKBZIGVCNUNBDSZNK/action/citation_signature","submit_replication":"https://pith.science/pith/SSUVTBIGNOKBZIGVCNUNBDSZNK/action/replication_record"}},"created_at":"2026-05-18T01:46:56.912205+00:00","updated_at":"2026-05-18T01:46:56.912205+00:00"}