{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:LIKOSIEGYG7DSMILUGYUFJAOC2","short_pith_number":"pith:LIKOSIEG","schema_version":"1.0","canonical_sha256":"5a14e92086c1be39310ba1b142a40e169140929bcb266b77d8257fba6e47324b","source":{"kind":"arxiv","id":"2110.15657","version":1},"attestation_state":"computed","paper":{"title":"Asymptotic Symmetry of Four Dimensional Einstein-Yang-Mills and Einstein-Maxwell Theory","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Nabamita Banerjee, Ranveer Kumar Singh, Tabasum Rahnuma","submitted_at":"2021-10-29T10:01:16Z","abstract_excerpt":"Asymptotic symmetry plays an important role in determining physical observables of a theory. Recently, in the context of four dimensional asymptotically flat pure gravity and $\\mathcal{N}=1$ supergravity, it has been proposed that OPEs of appropriate celestial amplitudes can be used to find their asymptotic symmetries. In this paper we find the asymptotic symmetry algebras of four dimensional Einstein-Yang-Mills and Einstein-Maxwell theories using this alternative approach, namely using the OPEs of their respective celestial amplitudes. The algebra obtained here are in agreement with the known"},"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":"2110.15657","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"hep-th","submitted_at":"2021-10-29T10:01:16Z","cross_cats_sorted":[],"title_canon_sha256":"4d2474dbd939d35ffe022d2cd737f148045ccacd4cd6c1a51b34fe83c6cb30e4","abstract_canon_sha256":"ed32877f81449d83b1e384849bafbb1b8077cb72ab0f12dab42655eee43e359f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:51:11.209642Z","signature_b64":"fJ0YXcr03L7qVU+3wkl7EDMlHAdtdRRLquf5At53qQGYp1Nw2YxQhPxY1qecQwpDtb/zs3ct0nykyyeeJ75SAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5a14e92086c1be39310ba1b142a40e169140929bcb266b77d8257fba6e47324b","last_reissued_at":"2026-07-05T03:51:11.209167Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:51:11.209167Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Asymptotic Symmetry of Four Dimensional Einstein-Yang-Mills and Einstein-Maxwell Theory","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Nabamita Banerjee, Ranveer Kumar Singh, Tabasum Rahnuma","submitted_at":"2021-10-29T10:01:16Z","abstract_excerpt":"Asymptotic symmetry plays an important role in determining physical observables of a theory. Recently, in the context of four dimensional asymptotically flat pure gravity and $\\mathcal{N}=1$ supergravity, it has been proposed that OPEs of appropriate celestial amplitudes can be used to find their asymptotic symmetries. In this paper we find the asymptotic symmetry algebras of four dimensional Einstein-Yang-Mills and Einstein-Maxwell theories using this alternative approach, namely using the OPEs of their respective celestial amplitudes. The algebra obtained here are in agreement with the known"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.15657","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/2110.15657/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":"2110.15657","created_at":"2026-07-05T03:51:11.209225+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.15657v1","created_at":"2026-07-05T03:51:11.209225+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.15657","created_at":"2026-07-05T03:51:11.209225+00:00"},{"alias_kind":"pith_short_12","alias_value":"LIKOSIEGYG7D","created_at":"2026-07-05T03:51:11.209225+00:00"},{"alias_kind":"pith_short_16","alias_value":"LIKOSIEGYG7DSMIL","created_at":"2026-07-05T03:51:11.209225+00:00"},{"alias_kind":"pith_short_8","alias_value":"LIKOSIEG","created_at":"2026-07-05T03:51:11.209225+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.19253","citing_title":"AdS S-Matrix for Massive Vector Fields","ref_index":52,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LIKOSIEGYG7DSMILUGYUFJAOC2","json":"https://pith.science/pith/LIKOSIEGYG7DSMILUGYUFJAOC2.json","graph_json":"https://pith.science/api/pith-number/LIKOSIEGYG7DSMILUGYUFJAOC2/graph.json","events_json":"https://pith.science/api/pith-number/LIKOSIEGYG7DSMILUGYUFJAOC2/events.json","paper":"https://pith.science/paper/LIKOSIEG"},"agent_actions":{"view_html":"https://pith.science/pith/LIKOSIEGYG7DSMILUGYUFJAOC2","download_json":"https://pith.science/pith/LIKOSIEGYG7DSMILUGYUFJAOC2.json","view_paper":"https://pith.science/paper/LIKOSIEG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.15657&json=true","fetch_graph":"https://pith.science/api/pith-number/LIKOSIEGYG7DSMILUGYUFJAOC2/graph.json","fetch_events":"https://pith.science/api/pith-number/LIKOSIEGYG7DSMILUGYUFJAOC2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LIKOSIEGYG7DSMILUGYUFJAOC2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LIKOSIEGYG7DSMILUGYUFJAOC2/action/storage_attestation","attest_author":"https://pith.science/pith/LIKOSIEGYG7DSMILUGYUFJAOC2/action/author_attestation","sign_citation":"https://pith.science/pith/LIKOSIEGYG7DSMILUGYUFJAOC2/action/citation_signature","submit_replication":"https://pith.science/pith/LIKOSIEGYG7DSMILUGYUFJAOC2/action/replication_record"}},"created_at":"2026-07-05T03:51:11.209225+00:00","updated_at":"2026-07-05T03:51:11.209225+00:00"}