{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:2LYJL27F4X56AWWP6YV5D73F4B","short_pith_number":"pith:2LYJL27F","schema_version":"1.0","canonical_sha256":"d2f095ebe5e5fbe05acff62bd1ff65e05289f675cb7fad0c384fa6bb0449ca4d","source":{"kind":"arxiv","id":"2506.14505","version":2},"attestation_state":"computed","paper":{"title":"Holography of a novel codimension-2 defect CFT","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dimitrios Zoakos, George Georgiou, Georgios Linardopoulos","submitted_at":"2025-06-17T13:29:16Z","abstract_excerpt":"We propose and study a new holographic duality between a non-supersymmetric defect conformal field theory (dCFT) and its gravity dual. On the gravity side, the defect is realised by a novel solution of a D5 probe brane embedded in the $AdS_5\\times S^5$ geometry. The D5 brane wraps an $S^2\\subset S^5$ and accommodates $k$ units of flux through the $S^2$. The symmetry of the induced on the brane metric is $AdS_3\\times S^1\\times S^2$. The brane ends on an $\\mathbb{R}^{(1,1)}$ subspace of the 4-dimensional $AdS_5$ boundary resulting to a codimension-2 defect. We first prove that our brane configur"},"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":"2506.14505","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-06-17T13:29:16Z","cross_cats_sorted":[],"title_canon_sha256":"c40952bb39e2dc61743469188eecfb46be51eb91f11b25b955a25ca295228aae","abstract_canon_sha256":"57c3f8a126e784322aec9b1cd10c36efa4157aedf0b7eb87a63e89056dc5408a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:09:44.847895Z","signature_b64":"433Ij0t1jVQLJn04KSEwh/tb7Nub8Xx2198/S/UgTNYn4JtPdG5DIBcgIhK03vZZZ0V9nUFLExBCyjQjyZlIBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d2f095ebe5e5fbe05acff62bd1ff65e05289f675cb7fad0c384fa6bb0449ca4d","last_reissued_at":"2026-07-05T12:09:44.847348Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:09:44.847348Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holography of a novel codimension-2 defect CFT","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dimitrios Zoakos, George Georgiou, Georgios Linardopoulos","submitted_at":"2025-06-17T13:29:16Z","abstract_excerpt":"We propose and study a new holographic duality between a non-supersymmetric defect conformal field theory (dCFT) and its gravity dual. On the gravity side, the defect is realised by a novel solution of a D5 probe brane embedded in the $AdS_5\\times S^5$ geometry. The D5 brane wraps an $S^2\\subset S^5$ and accommodates $k$ units of flux through the $S^2$. The symmetry of the induced on the brane metric is $AdS_3\\times S^1\\times S^2$. The brane ends on an $\\mathbb{R}^{(1,1)}$ subspace of the 4-dimensional $AdS_5$ boundary resulting to a codimension-2 defect. We first prove that our brane configur"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.14505","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/2506.14505/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":"2506.14505","created_at":"2026-07-05T12:09:44.847411+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.14505v2","created_at":"2026-07-05T12:09:44.847411+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.14505","created_at":"2026-07-05T12:09:44.847411+00:00"},{"alias_kind":"pith_short_12","alias_value":"2LYJL27F4X56","created_at":"2026-07-05T12:09:44.847411+00:00"},{"alias_kind":"pith_short_16","alias_value":"2LYJL27F4X56AWWP","created_at":"2026-07-05T12:09:44.847411+00:00"},{"alias_kind":"pith_short_8","alias_value":"2LYJL27F","created_at":"2026-07-05T12:09:44.847411+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.14726","citing_title":"Holographic interpolations of codimension-2 defect CFTs","ref_index":2,"is_internal_anchor":false},{"citing_arxiv_id":"2605.27256","citing_title":"Thermal conformal partial waves from flat-space and defect CFT","ref_index":105,"is_internal_anchor":false},{"citing_arxiv_id":"2512.14853","citing_title":"Holographic interpolations of defect CFTs","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2601.15736","citing_title":"Heavy holographic correlators in defect conformal field theories","ref_index":34,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19881","citing_title":"Weyl Anomaly Coefficients of Holographic Defect CFTs at Weak and Strong Coupling","ref_index":1,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2LYJL27F4X56AWWP6YV5D73F4B","json":"https://pith.science/pith/2LYJL27F4X56AWWP6YV5D73F4B.json","graph_json":"https://pith.science/api/pith-number/2LYJL27F4X56AWWP6YV5D73F4B/graph.json","events_json":"https://pith.science/api/pith-number/2LYJL27F4X56AWWP6YV5D73F4B/events.json","paper":"https://pith.science/paper/2LYJL27F"},"agent_actions":{"view_html":"https://pith.science/pith/2LYJL27F4X56AWWP6YV5D73F4B","download_json":"https://pith.science/pith/2LYJL27F4X56AWWP6YV5D73F4B.json","view_paper":"https://pith.science/paper/2LYJL27F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.14505&json=true","fetch_graph":"https://pith.science/api/pith-number/2LYJL27F4X56AWWP6YV5D73F4B/graph.json","fetch_events":"https://pith.science/api/pith-number/2LYJL27F4X56AWWP6YV5D73F4B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2LYJL27F4X56AWWP6YV5D73F4B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2LYJL27F4X56AWWP6YV5D73F4B/action/storage_attestation","attest_author":"https://pith.science/pith/2LYJL27F4X56AWWP6YV5D73F4B/action/author_attestation","sign_citation":"https://pith.science/pith/2LYJL27F4X56AWWP6YV5D73F4B/action/citation_signature","submit_replication":"https://pith.science/pith/2LYJL27F4X56AWWP6YV5D73F4B/action/replication_record"}},"created_at":"2026-07-05T12:09:44.847411+00:00","updated_at":"2026-07-05T12:09:44.847411+00:00"}