{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:ZOJBDWI76LCEQQRXQPVQ4MV7YE","short_pith_number":"pith:ZOJBDWI7","schema_version":"1.0","canonical_sha256":"cb9211d91ff2c448423783eb0e32bfc1221ee8acb4a875677b812866316cdbe6","source":{"kind":"arxiv","id":"2110.10160","version":2},"attestation_state":"computed","paper":{"title":"Scale vs. Conformal Invariance at the IR Fixed Point of Quantum Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Kara Farnsworth, Kurt Hinterbichler, Ondrej Hulik","submitted_at":"2021-10-19T18:00:00Z","abstract_excerpt":"We examine the question of scale vs. conformal invariance for the linearized Einstein-Hilbert action, which describes the IR fixed point of quantum gravity. In $D = 4$, although the action is not conformally invariant in the usual sense, we explicitly show that the theory is a conformal field theory at the level of correlation functions. In higher dimensions, we show that the theory is scale but not conformally invariant, but can be embedded into a larger non-unitary conformal field theory, analogous to what has been found for Maxwell theory in $D>4$. We give evidence that similar statements 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":"2110.10160","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-10-19T18:00:00Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"7ea25037135b25a1e5f5a8a888e0bf4ee263fb1fd9a5548d0a8078712ac65b54","abstract_canon_sha256":"8c775f245e90612fd4d097da0965e1eab1f557d40914c07a5a731bc5074e757a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:16:15.710405Z","signature_b64":"Oou4R+HQUuDdH0zIR4S+p+hqOtPFNHmz+rYId3guhoGpm7cG04xOTez3atzeLRLCwsk/TK1MkaxVg6dt7kW2Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cb9211d91ff2c448423783eb0e32bfc1221ee8acb4a875677b812866316cdbe6","last_reissued_at":"2026-07-05T04:16:15.709888Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:16:15.709888Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scale vs. Conformal Invariance at the IR Fixed Point of Quantum Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Kara Farnsworth, Kurt Hinterbichler, Ondrej Hulik","submitted_at":"2021-10-19T18:00:00Z","abstract_excerpt":"We examine the question of scale vs. conformal invariance for the linearized Einstein-Hilbert action, which describes the IR fixed point of quantum gravity. In $D = 4$, although the action is not conformally invariant in the usual sense, we explicitly show that the theory is a conformal field theory at the level of correlation functions. In higher dimensions, we show that the theory is scale but not conformally invariant, but can be embedded into a larger non-unitary conformal field theory, analogous to what has been found for Maxwell theory in $D>4$. We give evidence that similar statements a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.10160","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2110.10160/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":"2110.10160","created_at":"2026-07-05T04:16:15.709955+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.10160v2","created_at":"2026-07-05T04:16:15.709955+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.10160","created_at":"2026-07-05T04:16:15.709955+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZOJBDWI76LCE","created_at":"2026-07-05T04:16:15.709955+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZOJBDWI76LCEQQRX","created_at":"2026-07-05T04:16:15.709955+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZOJBDWI7","created_at":"2026-07-05T04:16:15.709955+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.11884","citing_title":"Manifest duality and Lorentz covariance for linearised gravity as edge modes","ref_index":39,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZOJBDWI76LCEQQRXQPVQ4MV7YE","json":"https://pith.science/pith/ZOJBDWI76LCEQQRXQPVQ4MV7YE.json","graph_json":"https://pith.science/api/pith-number/ZOJBDWI76LCEQQRXQPVQ4MV7YE/graph.json","events_json":"https://pith.science/api/pith-number/ZOJBDWI76LCEQQRXQPVQ4MV7YE/events.json","paper":"https://pith.science/paper/ZOJBDWI7"},"agent_actions":{"view_html":"https://pith.science/pith/ZOJBDWI76LCEQQRXQPVQ4MV7YE","download_json":"https://pith.science/pith/ZOJBDWI76LCEQQRXQPVQ4MV7YE.json","view_paper":"https://pith.science/paper/ZOJBDWI7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.10160&json=true","fetch_graph":"https://pith.science/api/pith-number/ZOJBDWI76LCEQQRXQPVQ4MV7YE/graph.json","fetch_events":"https://pith.science/api/pith-number/ZOJBDWI76LCEQQRXQPVQ4MV7YE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZOJBDWI76LCEQQRXQPVQ4MV7YE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZOJBDWI76LCEQQRXQPVQ4MV7YE/action/storage_attestation","attest_author":"https://pith.science/pith/ZOJBDWI76LCEQQRXQPVQ4MV7YE/action/author_attestation","sign_citation":"https://pith.science/pith/ZOJBDWI76LCEQQRXQPVQ4MV7YE/action/citation_signature","submit_replication":"https://pith.science/pith/ZOJBDWI76LCEQQRXQPVQ4MV7YE/action/replication_record"}},"created_at":"2026-07-05T04:16:15.709955+00:00","updated_at":"2026-07-05T04:16:15.709955+00:00"}