{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:VAL4S2CPZCQ6FBRE4S5CZK4UBT","short_pith_number":"pith:VAL4S2CP","schema_version":"1.0","canonical_sha256":"a817c9684fc8a1e28624e4ba2cab940cd2d1a8066f5971f2ea01dc723c1dc180","source":{"kind":"arxiv","id":"hep-th/0206107","version":1},"attestation_state":"computed","paper":{"title":"Rotating deformations of AdS_3\\times S^3, the orbifold CFT and strings in the pp-wave limit","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Oleg Lunin, Samir D. Mathur","submitted_at":"2002-06-12T16:46:21Z","abstract_excerpt":"We construct an exact metric which at short distances is the metric of massless particles in 5+1 spacetime (moving along a diameter of the sphere) and is AdS_3\\times S^3 at infinity. We also consider a set of a conical defect spacetimes which are locally AdS_3\\times S^3 and have the masses and charges of a special set of chiral primaries of the dual orbifold CFT. We find that excitation energies for a scalar field in the latter geometries agree exactly with the excitations in the corresponding CFT state created by twist operators: redshift in the geometry reproduces `long circle' physics in th"},"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":"hep-th/0206107","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-06-12T16:46:21Z","cross_cats_sorted":[],"title_canon_sha256":"42085a5ff510db7f5f00768be4c57cc91430a4b2e6a36da59d24c4b764448a2a","abstract_canon_sha256":"652b2a7e09773f773ca9066fc8604f3655ddcd2f388bbfe69ef09a88e0b9af8e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:35:23.583778Z","signature_b64":"ifm4Znx3jjACAANQKTs5kKQeCj+8ytJ+HYVmgnAFLBGApYi1oIFdxvsQMZq5n3wHA2hBdrjsZ07Xu9qMVfawCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a817c9684fc8a1e28624e4ba2cab940cd2d1a8066f5971f2ea01dc723c1dc180","last_reissued_at":"2026-05-18T04:35:23.583216Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:35:23.583216Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Rotating deformations of AdS_3\\times S^3, the orbifold CFT and strings in the pp-wave limit","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Oleg Lunin, Samir D. Mathur","submitted_at":"2002-06-12T16:46:21Z","abstract_excerpt":"We construct an exact metric which at short distances is the metric of massless particles in 5+1 spacetime (moving along a diameter of the sphere) and is AdS_3\\times S^3 at infinity. We also consider a set of a conical defect spacetimes which are locally AdS_3\\times S^3 and have the masses and charges of a special set of chiral primaries of the dual orbifold CFT. We find that excitation energies for a scalar field in the latter geometries agree exactly with the excitations in the corresponding CFT state created by twist operators: redshift in the geometry reproduces `long circle' physics in th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0206107","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":""},"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":"hep-th/0206107","created_at":"2026-05-18T04:35:23.583299+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0206107v1","created_at":"2026-05-18T04:35:23.583299+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0206107","created_at":"2026-05-18T04:35:23.583299+00:00"},{"alias_kind":"pith_short_12","alias_value":"VAL4S2CPZCQ6","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_16","alias_value":"VAL4S2CPZCQ6FBRE","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_8","alias_value":"VAL4S2CP","created_at":"2026-05-18T12:25:51.375804+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2105.11639","citing_title":"Interpolating between multi-center microstate geometries","ref_index":55,"is_internal_anchor":true},{"citing_arxiv_id":"2605.06465","citing_title":"Non-planar corrections in the symmetric orbifold","ref_index":5,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VAL4S2CPZCQ6FBRE4S5CZK4UBT","json":"https://pith.science/pith/VAL4S2CPZCQ6FBRE4S5CZK4UBT.json","graph_json":"https://pith.science/api/pith-number/VAL4S2CPZCQ6FBRE4S5CZK4UBT/graph.json","events_json":"https://pith.science/api/pith-number/VAL4S2CPZCQ6FBRE4S5CZK4UBT/events.json","paper":"https://pith.science/paper/VAL4S2CP"},"agent_actions":{"view_html":"https://pith.science/pith/VAL4S2CPZCQ6FBRE4S5CZK4UBT","download_json":"https://pith.science/pith/VAL4S2CPZCQ6FBRE4S5CZK4UBT.json","view_paper":"https://pith.science/paper/VAL4S2CP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0206107&json=true","fetch_graph":"https://pith.science/api/pith-number/VAL4S2CPZCQ6FBRE4S5CZK4UBT/graph.json","fetch_events":"https://pith.science/api/pith-number/VAL4S2CPZCQ6FBRE4S5CZK4UBT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VAL4S2CPZCQ6FBRE4S5CZK4UBT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VAL4S2CPZCQ6FBRE4S5CZK4UBT/action/storage_attestation","attest_author":"https://pith.science/pith/VAL4S2CPZCQ6FBRE4S5CZK4UBT/action/author_attestation","sign_citation":"https://pith.science/pith/VAL4S2CPZCQ6FBRE4S5CZK4UBT/action/citation_signature","submit_replication":"https://pith.science/pith/VAL4S2CPZCQ6FBRE4S5CZK4UBT/action/replication_record"}},"created_at":"2026-05-18T04:35:23.583299+00:00","updated_at":"2026-05-18T04:35:23.583299+00:00"}