{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:TKBNHEIE44PCNLIUEODVJZ25Y6","short_pith_number":"pith:TKBNHEIE","schema_version":"1.0","canonical_sha256":"9a82d39104e71e26ad14238754e75dc7950f1cd34316a55e55c92cd344aff272","source":{"kind":"arxiv","id":"2311.14797","version":1},"attestation_state":"computed","paper":{"title":"Quantum holographic surface anomalies","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Maxime Tr\\'epanier, Nadav Drukker, Omar Shahpo","submitted_at":"2023-11-24T19:00:01Z","abstract_excerpt":"Expectation values of surface operators suffer from logarithmic divergences reflecting a conformal anomaly. In a holographic setting, where surface operators can be computed by a minimal surface in $AdS$, the leading contribution to the anomaly comes from a divergence in the classical action (or area) of the minimal surface. We study the subleading correction to it due to quantum fluctuations of the minimal surface. In the same way that the divergence in the area does not require a global solution but only a near-boundary analysis, the same holds for the quantum corrections. We study the asymp"},"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":"2311.14797","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-11-24T19:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"7f951ecf7cd89e1c887ce74da99e99f1684e5122ec650707c7250851fa49f5ba","abstract_canon_sha256":"8a6618eb948051dade702f4424b393fe227037725d9789b2193c89b4760a11b1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:16:52.736774Z","signature_b64":"IXZrQBQRquGeGTWFlRhGbkltLeu9yZiUkOQAXzXVUH3WJ6QR9ZyVDbb3sc694EHQZgut0mIzQcR5DDXPmkWHBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a82d39104e71e26ad14238754e75dc7950f1cd34316a55e55c92cd344aff272","last_reissued_at":"2026-07-05T07:16:52.736360Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:16:52.736360Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum holographic surface anomalies","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Maxime Tr\\'epanier, Nadav Drukker, Omar Shahpo","submitted_at":"2023-11-24T19:00:01Z","abstract_excerpt":"Expectation values of surface operators suffer from logarithmic divergences reflecting a conformal anomaly. In a holographic setting, where surface operators can be computed by a minimal surface in $AdS$, the leading contribution to the anomaly comes from a divergence in the classical action (or area) of the minimal surface. We study the subleading correction to it due to quantum fluctuations of the minimal surface. In the same way that the divergence in the area does not require a global solution but only a near-boundary analysis, the same holds for the quantum corrections. We study the asymp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.14797","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/2311.14797/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":"2311.14797","created_at":"2026-07-05T07:16:52.736420+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.14797v1","created_at":"2026-07-05T07:16:52.736420+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.14797","created_at":"2026-07-05T07:16:52.736420+00:00"},{"alias_kind":"pith_short_12","alias_value":"TKBNHEIE44PC","created_at":"2026-07-05T07:16:52.736420+00:00"},{"alias_kind":"pith_short_16","alias_value":"TKBNHEIE44PCNLIU","created_at":"2026-07-05T07:16:52.736420+00:00"},{"alias_kind":"pith_short_8","alias_value":"TKBNHEIE","created_at":"2026-07-05T07:16:52.736420+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.06858","citing_title":"Non-planar corrections to ABJM Bremsstrahlung function from quantum M2 brane","ref_index":7,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TKBNHEIE44PCNLIUEODVJZ25Y6","json":"https://pith.science/pith/TKBNHEIE44PCNLIUEODVJZ25Y6.json","graph_json":"https://pith.science/api/pith-number/TKBNHEIE44PCNLIUEODVJZ25Y6/graph.json","events_json":"https://pith.science/api/pith-number/TKBNHEIE44PCNLIUEODVJZ25Y6/events.json","paper":"https://pith.science/paper/TKBNHEIE"},"agent_actions":{"view_html":"https://pith.science/pith/TKBNHEIE44PCNLIUEODVJZ25Y6","download_json":"https://pith.science/pith/TKBNHEIE44PCNLIUEODVJZ25Y6.json","view_paper":"https://pith.science/paper/TKBNHEIE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.14797&json=true","fetch_graph":"https://pith.science/api/pith-number/TKBNHEIE44PCNLIUEODVJZ25Y6/graph.json","fetch_events":"https://pith.science/api/pith-number/TKBNHEIE44PCNLIUEODVJZ25Y6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TKBNHEIE44PCNLIUEODVJZ25Y6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TKBNHEIE44PCNLIUEODVJZ25Y6/action/storage_attestation","attest_author":"https://pith.science/pith/TKBNHEIE44PCNLIUEODVJZ25Y6/action/author_attestation","sign_citation":"https://pith.science/pith/TKBNHEIE44PCNLIUEODVJZ25Y6/action/citation_signature","submit_replication":"https://pith.science/pith/TKBNHEIE44PCNLIUEODVJZ25Y6/action/replication_record"}},"created_at":"2026-07-05T07:16:52.736420+00:00","updated_at":"2026-07-05T07:16:52.736420+00:00"}