{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:PQLB7T74WEXTL47BB5CZ66HVX6","short_pith_number":"pith:PQLB7T74","schema_version":"1.0","canonical_sha256":"7c161fcffcb12f35f3e10f459f78f5bf9a15308c5575ef9abba57634089ee3c0","source":{"kind":"arxiv","id":"2005.08990","version":1},"attestation_state":"computed","paper":{"title":"Asymptotic Symmetries and Celestial CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Andrea Puhm, Laura Donnay, Sabrina Pasterski","submitted_at":"2020-05-18T18:00:06Z","abstract_excerpt":"We provide a unified treatment of conformally soft Goldstone modes which arise when spin-one or spin-two conformal primary wavefunctions become pure gauge for certain integer values of the conformal dimension $\\Delta$. This effort lands us at the crossroads of two ongoing debates about what the appropriate conformal basis for celestial CFT is and what the asymptotic symmetry group of Einstein gravity at null infinity should be. Finite energy wavefunctions are captured by the principal continuous series $\\Delta\\in 1+i\\mathbb{R}$ and form a complete basis. We show that conformal primaries with a"},"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":"2005.08990","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-05-18T18:00:06Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"d21883df4aa90f13f25197947c7521f63a4c9e944ca1bd54d79c1059b740c7a0","abstract_canon_sha256":"a4da7653b45dea2cba5c75d35541a02f686e76a54f0f54a26dd33c94148f0284"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:46:53.859109Z","signature_b64":"a8cYAVgLYQ3vQm70J3Odnj/WvmVv5Ub5a9vGGa5LXdvfYtG8T8dZ6KNcSfpwwIAUf9cRzA+PXgjcPKNfDP9vAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7c161fcffcb12f35f3e10f459f78f5bf9a15308c5575ef9abba57634089ee3c0","last_reissued_at":"2026-07-05T01:46:53.858674Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:46:53.858674Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Asymptotic Symmetries and Celestial CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Andrea Puhm, Laura Donnay, Sabrina Pasterski","submitted_at":"2020-05-18T18:00:06Z","abstract_excerpt":"We provide a unified treatment of conformally soft Goldstone modes which arise when spin-one or spin-two conformal primary wavefunctions become pure gauge for certain integer values of the conformal dimension $\\Delta$. This effort lands us at the crossroads of two ongoing debates about what the appropriate conformal basis for celestial CFT is and what the asymptotic symmetry group of Einstein gravity at null infinity should be. Finite energy wavefunctions are captured by the principal continuous series $\\Delta\\in 1+i\\mathbb{R}$ and form a complete basis. We show that conformal primaries with a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2005.08990","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/2005.08990/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":"2005.08990","created_at":"2026-07-05T01:46:53.858729+00:00"},{"alias_kind":"arxiv_version","alias_value":"2005.08990v1","created_at":"2026-07-05T01:46:53.858729+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2005.08990","created_at":"2026-07-05T01:46:53.858729+00:00"},{"alias_kind":"pith_short_12","alias_value":"PQLB7T74WEXT","created_at":"2026-07-05T01:46:53.858729+00:00"},{"alias_kind":"pith_short_16","alias_value":"PQLB7T74WEXTL47B","created_at":"2026-07-05T01:46:53.858729+00:00"},{"alias_kind":"pith_short_8","alias_value":"PQLB7T74","created_at":"2026-07-05T01:46:53.858729+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":12,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.24285","citing_title":"Topics in Celestial holography: A bottom-up perspective","ref_index":69,"is_internal_anchor":false},{"citing_arxiv_id":"2606.24285","citing_title":"Topics in Celestial holography: A bottom-up perspective","ref_index":70,"is_internal_anchor":false},{"citing_arxiv_id":"2606.05401","citing_title":"Carrollian holography with agentic AI: Real mass is imaginary","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02722","citing_title":"Asymptotically-FLRW$_3$ spacetimes","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2605.27870","citing_title":"Revisiting boundary electromagnetic duality and edge modes","ref_index":74,"is_internal_anchor":false},{"citing_arxiv_id":"2202.04702","citing_title":"Carrollian Perspective on Celestial Holography","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03250","citing_title":"Modular Flow of Celestial Conformal Field Theory","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2507.17811","citing_title":"Medicine show: A Calogero model with principal series states","ref_index":67,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03250","citing_title":"Modular Flow of Celestial Conformal Field Theory","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12854","citing_title":"Mixed-helicity bracket of celestial symmetries","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2604.09771","citing_title":"Towards a Carrollian Description of Yang-Mills","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03250","citing_title":"Modular Flow of Celestial Conformal Field Theory","ref_index":11,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PQLB7T74WEXTL47BB5CZ66HVX6","json":"https://pith.science/pith/PQLB7T74WEXTL47BB5CZ66HVX6.json","graph_json":"https://pith.science/api/pith-number/PQLB7T74WEXTL47BB5CZ66HVX6/graph.json","events_json":"https://pith.science/api/pith-number/PQLB7T74WEXTL47BB5CZ66HVX6/events.json","paper":"https://pith.science/paper/PQLB7T74"},"agent_actions":{"view_html":"https://pith.science/pith/PQLB7T74WEXTL47BB5CZ66HVX6","download_json":"https://pith.science/pith/PQLB7T74WEXTL47BB5CZ66HVX6.json","view_paper":"https://pith.science/paper/PQLB7T74","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2005.08990&json=true","fetch_graph":"https://pith.science/api/pith-number/PQLB7T74WEXTL47BB5CZ66HVX6/graph.json","fetch_events":"https://pith.science/api/pith-number/PQLB7T74WEXTL47BB5CZ66HVX6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PQLB7T74WEXTL47BB5CZ66HVX6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PQLB7T74WEXTL47BB5CZ66HVX6/action/storage_attestation","attest_author":"https://pith.science/pith/PQLB7T74WEXTL47BB5CZ66HVX6/action/author_attestation","sign_citation":"https://pith.science/pith/PQLB7T74WEXTL47BB5CZ66HVX6/action/citation_signature","submit_replication":"https://pith.science/pith/PQLB7T74WEXTL47BB5CZ66HVX6/action/replication_record"}},"created_at":"2026-07-05T01:46:53.858729+00:00","updated_at":"2026-07-05T01:46:53.858729+00:00"}