{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:FCM7BFOFN5U3MRTPSREUUBL5T3","short_pith_number":"pith:FCM7BFOF","schema_version":"1.0","canonical_sha256":"2899f095c56f69b6466f94494a057d9ef9f0af54f3be45562a6bd0f99ba0f9d7","source":{"kind":"arxiv","id":"2302.10222","version":1},"attestation_state":"computed","paper":{"title":"Symmetries in Celestial CFT$_d$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andrea Puhm, Emilio Trevisani, Yorgo Pano","submitted_at":"2023-02-20T19:01:29Z","abstract_excerpt":"We use tools from conformal representation theory to classify the symmetries associated to conformally soft operators in celestial CFT (CCFT) in general dimensions $d$. The conformal multiplets in $d>2$ take the form of celestial necklaces whose structure is much richer than the celestial diamonds in $d=2$, it depends on whether $d$ is even or odd and involves mixed-symmetric tensor representations of $SO(d)$. The existence of primary descendants in CCFT multiplets corresponds to (higher derivative) conservation equations for conformally soft operators. We lay out a unified method for construc"},"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":"2302.10222","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-02-20T19:01:29Z","cross_cats_sorted":[],"title_canon_sha256":"6e813b60dd5601cc8d6bc7e9102b868a8e15aa8f18437e9ac6df93d93dcea911","abstract_canon_sha256":"b8cdfefb570863aa1cc3372cd64d542bdc6f531f0714f0210db641d8da8ee823"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:36:29.798097Z","signature_b64":"gSorYLGeUUlq+XdLhcw8o7+jv3y0+5AOyqxTfkFCcuSUTAOwANAO1VkQemcWqUWIUHHfo2TNHrFl10agPwieAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2899f095c56f69b6466f94494a057d9ef9f0af54f3be45562a6bd0f99ba0f9d7","last_reissued_at":"2026-07-05T06:36:29.797570Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:36:29.797570Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Symmetries in Celestial CFT$_d$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andrea Puhm, Emilio Trevisani, Yorgo Pano","submitted_at":"2023-02-20T19:01:29Z","abstract_excerpt":"We use tools from conformal representation theory to classify the symmetries associated to conformally soft operators in celestial CFT (CCFT) in general dimensions $d$. The conformal multiplets in $d>2$ take the form of celestial necklaces whose structure is much richer than the celestial diamonds in $d=2$, it depends on whether $d$ is even or odd and involves mixed-symmetric tensor representations of $SO(d)$. The existence of primary descendants in CCFT multiplets corresponds to (higher derivative) conservation equations for conformally soft operators. We lay out a unified method for construc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2302.10222","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2302.10222/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":"2302.10222","created_at":"2026-07-05T06:36:29.797630+00:00"},{"alias_kind":"arxiv_version","alias_value":"2302.10222v1","created_at":"2026-07-05T06:36:29.797630+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2302.10222","created_at":"2026-07-05T06:36:29.797630+00:00"},{"alias_kind":"pith_short_12","alias_value":"FCM7BFOFN5U3","created_at":"2026-07-05T06:36:29.797630+00:00"},{"alias_kind":"pith_short_16","alias_value":"FCM7BFOFN5U3MRTP","created_at":"2026-07-05T06:36:29.797630+00:00"},{"alias_kind":"pith_short_8","alias_value":"FCM7BFOF","created_at":"2026-07-05T06:36:29.797630+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.16641","citing_title":"On bulk reconstruction in Lorentzian AdS and its flat space limit","ref_index":81,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12854","citing_title":"Mixed-helicity bracket of celestial symmetries","ref_index":105,"is_internal_anchor":false},{"citing_arxiv_id":"2604.11602","citing_title":"Celestial 1-form symmetries","ref_index":19,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FCM7BFOFN5U3MRTPSREUUBL5T3","json":"https://pith.science/pith/FCM7BFOFN5U3MRTPSREUUBL5T3.json","graph_json":"https://pith.science/api/pith-number/FCM7BFOFN5U3MRTPSREUUBL5T3/graph.json","events_json":"https://pith.science/api/pith-number/FCM7BFOFN5U3MRTPSREUUBL5T3/events.json","paper":"https://pith.science/paper/FCM7BFOF"},"agent_actions":{"view_html":"https://pith.science/pith/FCM7BFOFN5U3MRTPSREUUBL5T3","download_json":"https://pith.science/pith/FCM7BFOFN5U3MRTPSREUUBL5T3.json","view_paper":"https://pith.science/paper/FCM7BFOF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2302.10222&json=true","fetch_graph":"https://pith.science/api/pith-number/FCM7BFOFN5U3MRTPSREUUBL5T3/graph.json","fetch_events":"https://pith.science/api/pith-number/FCM7BFOFN5U3MRTPSREUUBL5T3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FCM7BFOFN5U3MRTPSREUUBL5T3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FCM7BFOFN5U3MRTPSREUUBL5T3/action/storage_attestation","attest_author":"https://pith.science/pith/FCM7BFOFN5U3MRTPSREUUBL5T3/action/author_attestation","sign_citation":"https://pith.science/pith/FCM7BFOFN5U3MRTPSREUUBL5T3/action/citation_signature","submit_replication":"https://pith.science/pith/FCM7BFOFN5U3MRTPSREUUBL5T3/action/replication_record"}},"created_at":"2026-07-05T06:36:29.797630+00:00","updated_at":"2026-07-05T06:36:29.797630+00:00"}