{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:O2KL7OR7EJ4EWNJNDAEGLPEY63","short_pith_number":"pith:O2KL7OR7","schema_version":"1.0","canonical_sha256":"7694bfba3f22784b352d180865bc98f6f3699a011d1a94085324c8d7a9eb79e9","source":{"kind":"arxiv","id":"2112.14648","version":2},"attestation_state":"computed","paper":{"title":"Mapping out the internal space in AdS/BCFT with Wilson loops","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Christoph F. Uhlemann, Lorenzo Coccia","submitted_at":"2021-12-29T16:51:34Z","abstract_excerpt":"We study Wilson loops in string theory realizations of AdS/BCFT and wedge holography. The field theories are based on 3d $\\mathcal N=4$ long quiver gauge theories engineered by D3, D5 and NS5 branes, and on BCFTs involving 4d $\\mathcal N=4$ SYM coupled to such 3d theories. The holographic duals have geometry $AdS_4\\times S^2\\times S^2$ warped over a strip. We identify the holographic representation of antisymmetric Wilson loops associated with individual 3d gauge nodes in terms of probe D5-branes. The expectation values obtained holographically are matched to supersymmetric localization comput"},"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":"2112.14648","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-12-29T16:51:34Z","cross_cats_sorted":[],"title_canon_sha256":"df3e3e9fe6b6e55c35be0c8b0396fd9730d64f07a56f63124622abbb989e19f4","abstract_canon_sha256":"cd9a17d071b7744b3a5c0c465b91c9b8576d092bd1e0864380c7bdb4616dfb88"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:13:49.033195Z","signature_b64":"q4/goEIPertfYnkbUtL/518eoI4htwm24xLtVN7CCJWHOEOpXAfa7wUgVQh++RB1wIFU4sgPTupSLJMgNEZWDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7694bfba3f22784b352d180865bc98f6f3699a011d1a94085324c8d7a9eb79e9","last_reissued_at":"2026-07-05T04:13:49.032762Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:13:49.032762Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Mapping out the internal space in AdS/BCFT with Wilson loops","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Christoph F. Uhlemann, Lorenzo Coccia","submitted_at":"2021-12-29T16:51:34Z","abstract_excerpt":"We study Wilson loops in string theory realizations of AdS/BCFT and wedge holography. The field theories are based on 3d $\\mathcal N=4$ long quiver gauge theories engineered by D3, D5 and NS5 branes, and on BCFTs involving 4d $\\mathcal N=4$ SYM coupled to such 3d theories. The holographic duals have geometry $AdS_4\\times S^2\\times S^2$ warped over a strip. We identify the holographic representation of antisymmetric Wilson loops associated with individual 3d gauge nodes in terms of probe D5-branes. The expectation values obtained holographically are matched to supersymmetric localization comput"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2112.14648","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/2112.14648/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":"2112.14648","created_at":"2026-07-05T04:13:49.032818+00:00"},{"alias_kind":"arxiv_version","alias_value":"2112.14648v2","created_at":"2026-07-05T04:13:49.032818+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2112.14648","created_at":"2026-07-05T04:13:49.032818+00:00"},{"alias_kind":"pith_short_12","alias_value":"O2KL7OR7EJ4E","created_at":"2026-07-05T04:13:49.032818+00:00"},{"alias_kind":"pith_short_16","alias_value":"O2KL7OR7EJ4EWNJN","created_at":"2026-07-05T04:13:49.032818+00:00"},{"alias_kind":"pith_short_8","alias_value":"O2KL7OR7","created_at":"2026-07-05T04:13:49.032818+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2510.02997","citing_title":"Quantum corrected black hole microstates and entropy","ref_index":25,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/O2KL7OR7EJ4EWNJNDAEGLPEY63","json":"https://pith.science/pith/O2KL7OR7EJ4EWNJNDAEGLPEY63.json","graph_json":"https://pith.science/api/pith-number/O2KL7OR7EJ4EWNJNDAEGLPEY63/graph.json","events_json":"https://pith.science/api/pith-number/O2KL7OR7EJ4EWNJNDAEGLPEY63/events.json","paper":"https://pith.science/paper/O2KL7OR7"},"agent_actions":{"view_html":"https://pith.science/pith/O2KL7OR7EJ4EWNJNDAEGLPEY63","download_json":"https://pith.science/pith/O2KL7OR7EJ4EWNJNDAEGLPEY63.json","view_paper":"https://pith.science/paper/O2KL7OR7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2112.14648&json=true","fetch_graph":"https://pith.science/api/pith-number/O2KL7OR7EJ4EWNJNDAEGLPEY63/graph.json","fetch_events":"https://pith.science/api/pith-number/O2KL7OR7EJ4EWNJNDAEGLPEY63/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/O2KL7OR7EJ4EWNJNDAEGLPEY63/action/timestamp_anchor","attest_storage":"https://pith.science/pith/O2KL7OR7EJ4EWNJNDAEGLPEY63/action/storage_attestation","attest_author":"https://pith.science/pith/O2KL7OR7EJ4EWNJNDAEGLPEY63/action/author_attestation","sign_citation":"https://pith.science/pith/O2KL7OR7EJ4EWNJNDAEGLPEY63/action/citation_signature","submit_replication":"https://pith.science/pith/O2KL7OR7EJ4EWNJNDAEGLPEY63/action/replication_record"}},"created_at":"2026-07-05T04:13:49.032818+00:00","updated_at":"2026-07-05T04:13:49.032818+00:00"}