{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:X64OLKA6ZDGN7H54T4KUUNV3B7","short_pith_number":"pith:X64OLKA6","schema_version":"1.0","canonical_sha256":"bfb8e5a81ec8ccdf9fbc9f154a36bb0fdd421077db328022724699b7fc0ba66c","source":{"kind":"arxiv","id":"1906.10715","version":2},"attestation_state":"computed","paper":{"title":"Information Transfer and Black Hole Evaporation via Traversable BTZ Wormholes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Sam van Leuven, Shinji Hirano, Yang Lei","submitted_at":"2019-06-25T18:22:05Z","abstract_excerpt":"We study traversable wormholes by considering the duality between BTZ black holes and two-dimensional conformal field theory on the thermofield double state. The BTZ black holes can be rendered traversable by a negative energy shock wave. Following Gao, Jafferis and Wall [1], we show that the negative energy shock wave is dual to the infinite boost limit of a specific double trace deformation which couples the left and right CFTs. We spell out the mechanism of information transfer through traversable BTZ wormholes, treating the backreaction of the message as a positive energy shockwave. The co"},"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":"1906.10715","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-06-25T18:22:05Z","cross_cats_sorted":[],"title_canon_sha256":"ad0458b8e8ad7b9496d5b1641496054bd2d2dc0aca3286a2c0a3d03efd66104a","abstract_canon_sha256":"66f3e65f704ef5f96d503fa8cafe423c19e6e01db02e2b456d568e973f47257e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:07:36.630703Z","signature_b64":"ASTMNGQUw3DpnpVaYiY/jH5Q6w5V8ZS4TkxIgP1SRVcy/jR1SAnuuTvo5WpqO7wbsP+Ge1sK52Raz/IEw+o+Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bfb8e5a81ec8ccdf9fbc9f154a36bb0fdd421077db328022724699b7fc0ba66c","last_reissued_at":"2026-07-05T00:07:36.630264Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:07:36.630264Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Information Transfer and Black Hole Evaporation via Traversable BTZ Wormholes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Sam van Leuven, Shinji Hirano, Yang Lei","submitted_at":"2019-06-25T18:22:05Z","abstract_excerpt":"We study traversable wormholes by considering the duality between BTZ black holes and two-dimensional conformal field theory on the thermofield double state. The BTZ black holes can be rendered traversable by a negative energy shock wave. Following Gao, Jafferis and Wall [1], we show that the negative energy shock wave is dual to the infinite boost limit of a specific double trace deformation which couples the left and right CFTs. We spell out the mechanism of information transfer through traversable BTZ wormholes, treating the backreaction of the message as a positive energy shockwave. The co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.10715","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/1906.10715/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":"1906.10715","created_at":"2026-07-05T00:07:36.630322+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.10715v2","created_at":"2026-07-05T00:07:36.630322+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.10715","created_at":"2026-07-05T00:07:36.630322+00:00"},{"alias_kind":"pith_short_12","alias_value":"X64OLKA6ZDGN","created_at":"2026-07-05T00:07:36.630322+00:00"},{"alias_kind":"pith_short_16","alias_value":"X64OLKA6ZDGN7H54","created_at":"2026-07-05T00:07:36.630322+00:00"},{"alias_kind":"pith_short_8","alias_value":"X64OLKA6","created_at":"2026-07-05T00:07:36.630322+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.01388","citing_title":"Quasinormal Modes and the Switchback Effect in Schwarzschild-de Sitter","ref_index":55,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X64OLKA6ZDGN7H54T4KUUNV3B7","json":"https://pith.science/pith/X64OLKA6ZDGN7H54T4KUUNV3B7.json","graph_json":"https://pith.science/api/pith-number/X64OLKA6ZDGN7H54T4KUUNV3B7/graph.json","events_json":"https://pith.science/api/pith-number/X64OLKA6ZDGN7H54T4KUUNV3B7/events.json","paper":"https://pith.science/paper/X64OLKA6"},"agent_actions":{"view_html":"https://pith.science/pith/X64OLKA6ZDGN7H54T4KUUNV3B7","download_json":"https://pith.science/pith/X64OLKA6ZDGN7H54T4KUUNV3B7.json","view_paper":"https://pith.science/paper/X64OLKA6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.10715&json=true","fetch_graph":"https://pith.science/api/pith-number/X64OLKA6ZDGN7H54T4KUUNV3B7/graph.json","fetch_events":"https://pith.science/api/pith-number/X64OLKA6ZDGN7H54T4KUUNV3B7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X64OLKA6ZDGN7H54T4KUUNV3B7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X64OLKA6ZDGN7H54T4KUUNV3B7/action/storage_attestation","attest_author":"https://pith.science/pith/X64OLKA6ZDGN7H54T4KUUNV3B7/action/author_attestation","sign_citation":"https://pith.science/pith/X64OLKA6ZDGN7H54T4KUUNV3B7/action/citation_signature","submit_replication":"https://pith.science/pith/X64OLKA6ZDGN7H54T4KUUNV3B7/action/replication_record"}},"created_at":"2026-07-05T00:07:36.630322+00:00","updated_at":"2026-07-05T00:07:36.630322+00:00"}