{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:EMOHHGABNJJR3TBYGTDWF2AFSP","short_pith_number":"pith:EMOHHGAB","schema_version":"1.0","canonical_sha256":"231c7398016a531dcc3834c762e80593feba84e6d0d08178a86ccaf0fe290308","source":{"kind":"arxiv","id":"1410.4543","version":3},"attestation_state":"computed","paper":{"title":"Effect of the deformation operator in the D1D5 CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"David Turton, Samir D. Mathur, Shaun Hampton, Zaq Carson","submitted_at":"2014-10-16T19:37:10Z","abstract_excerpt":"The D1D5 CFT gives a holographic dual description of a near-extremal black hole in string theory. The interaction in this theory is given by a marginal deformation operator, which is composed of supercharges acting on a twist operator. The twist operator links together different copies of a free CFT. We study the effect of this deformation operator when it links together CFT copies with winding numbers M and N to produce a copy with winding M+N, populated with excitations of a particular form. We compute the effect of the deformation operator in the full supersymmetric theory, firstly on a Ram"},"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":"1410.4543","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-16T19:37:10Z","cross_cats_sorted":[],"title_canon_sha256":"904e17ba916841eab13b7699b0dc842adab958000c8ae2ebbfe501fc74116d5a","abstract_canon_sha256":"973dd61a1fdfe553f2ff032d01a00ff15e868169f0c02c4879ae07d03d77bfb7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:26:38.691102Z","signature_b64":"wAVxqSddQsf7uTggqTb0Rqr3i8Ex5TVudXfuorOv8nKR894VmKAc/OiUrT7lh9HoFC7Lr+WZkjhwbemcc0/0AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"231c7398016a531dcc3834c762e80593feba84e6d0d08178a86ccaf0fe290308","last_reissued_at":"2026-05-18T02:26:38.690476Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:26:38.690476Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effect of the deformation operator in the D1D5 CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"David Turton, Samir D. Mathur, Shaun Hampton, Zaq Carson","submitted_at":"2014-10-16T19:37:10Z","abstract_excerpt":"The D1D5 CFT gives a holographic dual description of a near-extremal black hole in string theory. The interaction in this theory is given by a marginal deformation operator, which is composed of supercharges acting on a twist operator. The twist operator links together different copies of a free CFT. We study the effect of this deformation operator when it links together CFT copies with winding numbers M and N to produce a copy with winding M+N, populated with excitations of a particular form. We compute the effect of the deformation operator in the full supersymmetric theory, firstly on a Ram"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.4543","kind":"arxiv","version":3},"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":"1410.4543","created_at":"2026-05-18T02:26:38.690574+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.4543v3","created_at":"2026-05-18T02:26:38.690574+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.4543","created_at":"2026-05-18T02:26:38.690574+00:00"},{"alias_kind":"pith_short_12","alias_value":"EMOHHGABNJJR","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_16","alias_value":"EMOHHGABNJJR3TBY","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_8","alias_value":"EMOHHGAB","created_at":"2026-05-18T12:28:28.263976+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2603.18138","citing_title":"The Resolved Elliptic Genus and the D1-D5 CFT","ref_index":45,"is_internal_anchor":true},{"citing_arxiv_id":"2604.23287","citing_title":"Chaos of Berry curvature for BPS microstates","ref_index":100,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EMOHHGABNJJR3TBYGTDWF2AFSP","json":"https://pith.science/pith/EMOHHGABNJJR3TBYGTDWF2AFSP.json","graph_json":"https://pith.science/api/pith-number/EMOHHGABNJJR3TBYGTDWF2AFSP/graph.json","events_json":"https://pith.science/api/pith-number/EMOHHGABNJJR3TBYGTDWF2AFSP/events.json","paper":"https://pith.science/paper/EMOHHGAB"},"agent_actions":{"view_html":"https://pith.science/pith/EMOHHGABNJJR3TBYGTDWF2AFSP","download_json":"https://pith.science/pith/EMOHHGABNJJR3TBYGTDWF2AFSP.json","view_paper":"https://pith.science/paper/EMOHHGAB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.4543&json=true","fetch_graph":"https://pith.science/api/pith-number/EMOHHGABNJJR3TBYGTDWF2AFSP/graph.json","fetch_events":"https://pith.science/api/pith-number/EMOHHGABNJJR3TBYGTDWF2AFSP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EMOHHGABNJJR3TBYGTDWF2AFSP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EMOHHGABNJJR3TBYGTDWF2AFSP/action/storage_attestation","attest_author":"https://pith.science/pith/EMOHHGABNJJR3TBYGTDWF2AFSP/action/author_attestation","sign_citation":"https://pith.science/pith/EMOHHGABNJJR3TBYGTDWF2AFSP/action/citation_signature","submit_replication":"https://pith.science/pith/EMOHHGABNJJR3TBYGTDWF2AFSP/action/replication_record"}},"created_at":"2026-05-18T02:26:38.690574+00:00","updated_at":"2026-05-18T02:26:38.690574+00:00"}