{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:CA3KGCHBQE3634VRXRN6RIQAT7","short_pith_number":"pith:CA3KGCHB","schema_version":"1.0","canonical_sha256":"1036a308e18137edf2b1bc5be8a2009fd627e99aa9cdbb3d7c403f7db7904ce3","source":{"kind":"arxiv","id":"1811.10380","version":2},"attestation_state":"computed","paper":{"title":"Holographic Weyl anomaly for GJMS operators: one Laplacian to rule them all","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"D. E. D\\'iaz, F. Bugini","submitted_at":"2018-11-26T14:22:57Z","abstract_excerpt":"The holographic Weyl anomaly for GJMS operators (or conformal powers of the Laplacian) are obtained in four and six dimensions. In the context of AdS/CFT correspondence, free conformal scalars with higher-derivative kinetic operators are induced by an ordinary second-derivative massive bulk scalar. At one-loop quantum level, the duality dictionary for partition functions entails an equality between the functional determinants of the corresponding kinetic operators and, in particular, it provides a holographic route to their Weyl anomalies. The heat kernel of a single bulk massive scalar field "},"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":"1811.10380","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-11-26T14:22:57Z","cross_cats_sorted":["gr-qc","math-ph","math.MP"],"title_canon_sha256":"988f280ec5b746b4361d748e29608cc894ef6b0b77e1be1e7709d0b78b7041ca","abstract_canon_sha256":"743a9af9f5b610be1d3cf266bb618523714e0510b19cb9717922db64dfdc0ce8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:11.204251Z","signature_b64":"q/GSwPy13JbFiLUM1zWR/QKV22fSFwvoxwyIqEOVl6ITCnKTOQjciGoWiE5CUj0aAm0rnvwGQHnZjQq+Kre+Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1036a308e18137edf2b1bc5be8a2009fd627e99aa9cdbb3d7c403f7db7904ce3","last_reissued_at":"2026-05-17T23:50:11.203797Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:11.203797Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic Weyl anomaly for GJMS operators: one Laplacian to rule them all","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"D. E. D\\'iaz, F. Bugini","submitted_at":"2018-11-26T14:22:57Z","abstract_excerpt":"The holographic Weyl anomaly for GJMS operators (or conformal powers of the Laplacian) are obtained in four and six dimensions. In the context of AdS/CFT correspondence, free conformal scalars with higher-derivative kinetic operators are induced by an ordinary second-derivative massive bulk scalar. At one-loop quantum level, the duality dictionary for partition functions entails an equality between the functional determinants of the corresponding kinetic operators and, in particular, it provides a holographic route to their Weyl anomalies. The heat kernel of a single bulk massive scalar field "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.10380","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":""},"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":"1811.10380","created_at":"2026-05-17T23:50:11.203866+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.10380v2","created_at":"2026-05-17T23:50:11.203866+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.10380","created_at":"2026-05-17T23:50:11.203866+00:00"},{"alias_kind":"pith_short_12","alias_value":"CA3KGCHBQE36","created_at":"2026-05-18T12:32:16.446611+00:00"},{"alias_kind":"pith_short_16","alias_value":"CA3KGCHBQE3634VR","created_at":"2026-05-18T12:32:16.446611+00:00"},{"alias_kind":"pith_short_8","alias_value":"CA3KGCHB","created_at":"2026-05-18T12:32:16.446611+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CA3KGCHBQE3634VRXRN6RIQAT7","json":"https://pith.science/pith/CA3KGCHBQE3634VRXRN6RIQAT7.json","graph_json":"https://pith.science/api/pith-number/CA3KGCHBQE3634VRXRN6RIQAT7/graph.json","events_json":"https://pith.science/api/pith-number/CA3KGCHBQE3634VRXRN6RIQAT7/events.json","paper":"https://pith.science/paper/CA3KGCHB"},"agent_actions":{"view_html":"https://pith.science/pith/CA3KGCHBQE3634VRXRN6RIQAT7","download_json":"https://pith.science/pith/CA3KGCHBQE3634VRXRN6RIQAT7.json","view_paper":"https://pith.science/paper/CA3KGCHB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.10380&json=true","fetch_graph":"https://pith.science/api/pith-number/CA3KGCHBQE3634VRXRN6RIQAT7/graph.json","fetch_events":"https://pith.science/api/pith-number/CA3KGCHBQE3634VRXRN6RIQAT7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CA3KGCHBQE3634VRXRN6RIQAT7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CA3KGCHBQE3634VRXRN6RIQAT7/action/storage_attestation","attest_author":"https://pith.science/pith/CA3KGCHBQE3634VRXRN6RIQAT7/action/author_attestation","sign_citation":"https://pith.science/pith/CA3KGCHBQE3634VRXRN6RIQAT7/action/citation_signature","submit_replication":"https://pith.science/pith/CA3KGCHBQE3634VRXRN6RIQAT7/action/replication_record"}},"created_at":"2026-05-17T23:50:11.203866+00:00","updated_at":"2026-05-17T23:50:11.203866+00:00"}