{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:V3KSTVQZJHVZBZTVYM77QSHPPN","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"aeebf60815aab44b562c6a8316eda37ed33f403a1ebd901e61e217fd0e61c27a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-03-30T18:03:39Z","title_canon_sha256":"22397c471374aebb0d71907be68081e23fcb4b8f79ddec1168e006c10f717469"},"schema_version":"1.0","source":{"id":"2603.28880","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2603.28880","created_at":"2026-07-02T01:18:07Z"},{"alias_kind":"arxiv_version","alias_value":"2603.28880v4","created_at":"2026-07-02T01:18:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.28880","created_at":"2026-07-02T01:18:07Z"},{"alias_kind":"pith_short_12","alias_value":"V3KSTVQZJHVZ","created_at":"2026-07-02T01:18:07Z"},{"alias_kind":"pith_short_16","alias_value":"V3KSTVQZJHVZBZTV","created_at":"2026-07-02T01:18:07Z"},{"alias_kind":"pith_short_8","alias_value":"V3KSTVQZ","created_at":"2026-07-02T01:18:07Z"}],"graph_snapshots":[{"event_id":"sha256:44c1b664e250066555157811c373309e6141026eb5cab9f84d5528f0bcf5def3","target":"graph","created_at":"2026-07-02T01:18:07Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"We argue that the D3-brane action for the giant gravitons (as well as for their 1/4- and 1/8-BPS counterparts) should contain additional boundary terms which arise naturally from the path integral and which are required to make the variational problem well-defined. We derive the form of these terms and show that the corrected action has an on-shell value that reproduces the two-point function of the gauge theory operators."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The assumption that the additional boundary terms arise naturally from the path integral, are required to make the variational problem well-defined, and that the on-shell value of the corrected action directly reproduces the gauge theory two-point function without further corrections or normalizations."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Corrected D3-brane actions with path-integral boundary terms reproduce two-point functions of giant graviton operators, while GHY boundary terms yield correlators for Δ~N² operators in LLM geometries."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"The D3-brane action requires additional boundary terms to compute holographic two-point functions of heavy operators correctly."}],"snapshot_sha256":"9512d2ac9b57d07172e62f9640a7b1134a49735d2bbe680e08517786e7bb3fda"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"2569976982f28896aa565b53cd3f8c1016549804c0cf8b2c8e1c90b811eb1552"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2603.28880/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this paper we investigate the holographic computation of the two-point functions of $\\frac{1}{2}$-BPS chiral primary operators with scaling dimensions $\\Delta \\sim N$ or $\\Delta \\sim N^2$ in $\\mathcal{N}=4$ $SU(N)$ SYM using Type IIB supergravity. First we consider giant graviton operators, resolving ambiguities in the previous literature on holographic computation of the two-point function, and make a new proposal for this calculation. We argue that the D3-brane action for the giant gravitons (as well as for their $\\frac{1}{4}$- and $\\frac{1}{8}$-BPS counterparts) should contain additional","authors_text":"Prokopii Anempodistov","cross_cats":[],"headline":"The D3-brane action requires additional boundary terms to compute holographic two-point functions of heavy operators correctly.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-03-30T18:03:39Z","title":"Holographic two-point functions of heavy operators revisited"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.28880","kind":"arxiv","version":4},"verdict":{"created_at":"2026-05-14T00:48:40.206350Z","id":"c183a48c-4c17-448e-a655-fc32a648e7db","model_set":{"reader":"grok-4.3"},"one_line_summary":"Corrected D3-brane actions with path-integral boundary terms reproduce two-point functions of giant graviton operators, while GHY boundary terms yield correlators for Δ~N² operators in LLM geometries.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"The D3-brane action requires additional boundary terms to compute holographic two-point functions of heavy operators correctly.","strongest_claim":"We argue that the D3-brane action for the giant gravitons (as well as for their 1/4- and 1/8-BPS counterparts) should contain additional boundary terms which arise naturally from the path integral and which are required to make the variational problem well-defined. We derive the form of these terms and show that the corrected action has an on-shell value that reproduces the two-point function of the gauge theory operators.","weakest_assumption":"The assumption that the additional boundary terms arise naturally from the path integral, are required to make the variational problem well-defined, and that the on-shell value of the corrected action directly reproduces the gauge theory two-point function without further corrections or normalizations."}},"verdict_id":"c183a48c-4c17-448e-a655-fc32a648e7db"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:42efd1891eab214ed7041e79b47afee25d035e2549b51cf653c8d0e48908867d","target":"record","created_at":"2026-07-02T01:18:07Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"aeebf60815aab44b562c6a8316eda37ed33f403a1ebd901e61e217fd0e61c27a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-03-30T18:03:39Z","title_canon_sha256":"22397c471374aebb0d71907be68081e23fcb4b8f79ddec1168e006c10f717469"},"schema_version":"1.0","source":{"id":"2603.28880","kind":"arxiv","version":4}},"canonical_sha256":"aed529d61949eb90e675c33ff848ef7b4111b4f6c3375c2f18391e7aab10c0f6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aed529d61949eb90e675c33ff848ef7b4111b4f6c3375c2f18391e7aab10c0f6","first_computed_at":"2026-07-02T01:18:07.809730Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-02T01:18:07.809730Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4Yq6HfCHWVRcKNySn/JgxwhVIHdomXG5/tlFlAthbCtkGtL/EVX3Zkm8EAhNuSnrd+1/YLVPuBLk9CuB+MmgBw==","signature_status":"signed_v1","signed_at":"2026-07-02T01:18:07.810072Z","signed_message":"canonical_sha256_bytes"},"source_id":"2603.28880","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:42efd1891eab214ed7041e79b47afee25d035e2549b51cf653c8d0e48908867d","sha256:44c1b664e250066555157811c373309e6141026eb5cab9f84d5528f0bcf5def3"],"state_sha256":"e17c3c668679c7e87ac05c22662c288a3666c0fa51e4db9f97fc038107325c65"}