{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U","short_pith_number":"pith:5JX6Y6TQ","schema_version":"1.0","canonical_sha256":"ea6fec7a701780e4edd5ba1dbc8c59d520c2e572860589132ad9406ddd000aaa","source":{"kind":"arxiv","id":"1501.02260","version":3},"attestation_state":"computed","paper":{"title":"Worldline approach to semi-classical conformal blocks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Eliot Hijano, Per Kraus, River Snively","submitted_at":"2015-01-09T20:46:44Z","abstract_excerpt":"We extend recent results on semi-classical conformal blocks in 2d CFT and their relation to 3D gravity via the AdS/CFT correspondence. We consider four-point functions with two heavy and two light external operators, along with the exchange of a light operator. By explicit computation, we establish precise agreement between these CFT objects and a simple picture of particle worldlines joined by cubic vertices propagating in asymptotically AdS$_3$ geometries (conical defects or BTZ black holes). We provide a simple argument that explains this agreement."},"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":"1501.02260","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-01-09T20:46:44Z","cross_cats_sorted":[],"title_canon_sha256":"633b9540ad3d5259a00c69b5559e67d9081474da3c54b1b3c084276166bc1180","abstract_canon_sha256":"d089365282f800fdfb151c83dc096bdfd46b35e36b1d4bcf887e9d5804dec173"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:17:54.305332Z","signature_b64":"ppO9ZjD1ZxJt0YApaxuEGWfzqPuZOKPxUnVnViEIEPCo6ZAfuxXvS8JUjeqTXRhGg+vJkoJOd41kRYCSLkVSAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ea6fec7a701780e4edd5ba1dbc8c59d520c2e572860589132ad9406ddd000aaa","last_reissued_at":"2026-05-18T02:17:54.304752Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:17:54.304752Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Worldline approach to semi-classical conformal blocks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Eliot Hijano, Per Kraus, River Snively","submitted_at":"2015-01-09T20:46:44Z","abstract_excerpt":"We extend recent results on semi-classical conformal blocks in 2d CFT and their relation to 3D gravity via the AdS/CFT correspondence. We consider four-point functions with two heavy and two light external operators, along with the exchange of a light operator. By explicit computation, we establish precise agreement between these CFT objects and a simple picture of particle worldlines joined by cubic vertices propagating in asymptotically AdS$_3$ geometries (conical defects or BTZ black holes). We provide a simple argument that explains this agreement."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.02260","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":"1501.02260","created_at":"2026-05-18T02:17:54.304852+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.02260v3","created_at":"2026-05-18T02:17:54.304852+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.02260","created_at":"2026-05-18T02:17:54.304852+00:00"},{"alias_kind":"pith_short_12","alias_value":"5JX6Y6TQC6AO","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_16","alias_value":"5JX6Y6TQC6AOJ3OV","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_8","alias_value":"5JX6Y6TQ","created_at":"2026-05-18T12:29:05.191682+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1906.08405","citing_title":"Propagator identities, holographic conformal blocks, and higher-point AdS diagrams","ref_index":93,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U","json":"https://pith.science/pith/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U.json","graph_json":"https://pith.science/api/pith-number/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U/graph.json","events_json":"https://pith.science/api/pith-number/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U/events.json","paper":"https://pith.science/paper/5JX6Y6TQ"},"agent_actions":{"view_html":"https://pith.science/pith/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U","download_json":"https://pith.science/pith/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U.json","view_paper":"https://pith.science/paper/5JX6Y6TQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.02260&json=true","fetch_graph":"https://pith.science/api/pith-number/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U/graph.json","fetch_events":"https://pith.science/api/pith-number/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U/action/storage_attestation","attest_author":"https://pith.science/pith/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U/action/author_attestation","sign_citation":"https://pith.science/pith/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U/action/citation_signature","submit_replication":"https://pith.science/pith/5JX6Y6TQC6AOJ3OVXIO3ZDCZ2U/action/replication_record"}},"created_at":"2026-05-18T02:17:54.304852+00:00","updated_at":"2026-05-18T02:17:54.304852+00:00"}