{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:RZMFO3E3RB3QS2W3G7XXLWJD3P","short_pith_number":"pith:RZMFO3E3","schema_version":"1.0","canonical_sha256":"8e58576c9b8877096adb37ef75d923dbc1efdf81ff4df0ee48c57375ca90ac22","source":{"kind":"arxiv","id":"1402.4486","version":3},"attestation_state":"computed","paper":{"title":"Finite higher spin transformations from exponentiation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Samuel Monnier","submitted_at":"2014-02-18T21:00:38Z","abstract_excerpt":"We study the exponentiation of elements of the gauge Lie algebras ${\\rm hs}(\\lambda)$ of three-dimensional higher spin theories. Exponentiable elements generate one-parameter groups of finite higher spin symmetries. We show that elements of ${\\rm hs}(\\lambda)$ in a dense set are exponentiable, when pictured in certain representations of ${\\rm hs}(\\lambda)$, induced from representations of $SL(2,\\mathbb{R})$ in the complementary series. We also provide a geometric picture of higher spin gauge transformations clarifying the physical origin of these representations. This allows us to construct an"},"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":"1402.4486","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-18T21:00:38Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"b59f91ce61d81b98d2719a5a9ea7e680a349750155e830c7295e4160c8923825","abstract_canon_sha256":"d647d02afb0a31f64781ca122aaa36e08b3a432ac81ab6328bc489431cdea525"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:20:59.460163Z","signature_b64":"vUCkMTy6qOwyQAlFsS1tYgiDUCq7yKOGKvxmy77TSxsMam62GMw4AyhEj9nr8MRjXon2mQHoTiYkinneO12GCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e58576c9b8877096adb37ef75d923dbc1efdf81ff4df0ee48c57375ca90ac22","last_reissued_at":"2026-05-18T02:20:59.459602Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:20:59.459602Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite higher spin transformations from exponentiation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Samuel Monnier","submitted_at":"2014-02-18T21:00:38Z","abstract_excerpt":"We study the exponentiation of elements of the gauge Lie algebras ${\\rm hs}(\\lambda)$ of three-dimensional higher spin theories. Exponentiable elements generate one-parameter groups of finite higher spin symmetries. We show that elements of ${\\rm hs}(\\lambda)$ in a dense set are exponentiable, when pictured in certain representations of ${\\rm hs}(\\lambda)$, induced from representations of $SL(2,\\mathbb{R})$ in the complementary series. We also provide a geometric picture of higher spin gauge transformations clarifying the physical origin of these representations. This allows us to construct an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.4486","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":""},"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":"1402.4486","created_at":"2026-05-18T02:20:59.459680+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.4486v3","created_at":"2026-05-18T02:20:59.459680+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.4486","created_at":"2026-05-18T02:20:59.459680+00:00"},{"alias_kind":"pith_short_12","alias_value":"RZMFO3E3RB3Q","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_16","alias_value":"RZMFO3E3RB3QS2W3","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_8","alias_value":"RZMFO3E3","created_at":"2026-05-18T12:28:46.137349+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2602.19812","citing_title":"dS$^4$ Metamorphosis","ref_index":81,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RZMFO3E3RB3QS2W3G7XXLWJD3P","json":"https://pith.science/pith/RZMFO3E3RB3QS2W3G7XXLWJD3P.json","graph_json":"https://pith.science/api/pith-number/RZMFO3E3RB3QS2W3G7XXLWJD3P/graph.json","events_json":"https://pith.science/api/pith-number/RZMFO3E3RB3QS2W3G7XXLWJD3P/events.json","paper":"https://pith.science/paper/RZMFO3E3"},"agent_actions":{"view_html":"https://pith.science/pith/RZMFO3E3RB3QS2W3G7XXLWJD3P","download_json":"https://pith.science/pith/RZMFO3E3RB3QS2W3G7XXLWJD3P.json","view_paper":"https://pith.science/paper/RZMFO3E3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.4486&json=true","fetch_graph":"https://pith.science/api/pith-number/RZMFO3E3RB3QS2W3G7XXLWJD3P/graph.json","fetch_events":"https://pith.science/api/pith-number/RZMFO3E3RB3QS2W3G7XXLWJD3P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RZMFO3E3RB3QS2W3G7XXLWJD3P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RZMFO3E3RB3QS2W3G7XXLWJD3P/action/storage_attestation","attest_author":"https://pith.science/pith/RZMFO3E3RB3QS2W3G7XXLWJD3P/action/author_attestation","sign_citation":"https://pith.science/pith/RZMFO3E3RB3QS2W3G7XXLWJD3P/action/citation_signature","submit_replication":"https://pith.science/pith/RZMFO3E3RB3QS2W3G7XXLWJD3P/action/replication_record"}},"created_at":"2026-05-18T02:20:59.459680+00:00","updated_at":"2026-05-18T02:20:59.459680+00:00"}