{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:YULG2JI2LLLOGAI4DMPQRQ5JRN","short_pith_number":"pith:YULG2JI2","canonical_record":{"source":{"id":"1212.4553","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2012-12-19T01:44:10Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"2d442dd7a10a4cd6e483d7a0cfcd8b51d8313ac43308c1c8cc86cfecd1d7b4c5","abstract_canon_sha256":"729fbc70cd3bface77d88341ed4bdc7f1121aee14f2058566bdb293579e21270"},"schema_version":"1.0"},"canonical_sha256":"c5166d251a5ad6e3011c1b1f08c3a98b6f5d7fbf83d9c9e7614b636b9de6e67a","source":{"kind":"arxiv","id":"1212.4553","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.4553","created_at":"2026-05-18T03:36:17Z"},{"alias_kind":"arxiv_version","alias_value":"1212.4553v3","created_at":"2026-05-18T03:36:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.4553","created_at":"2026-05-18T03:36:17Z"},{"alias_kind":"pith_short_12","alias_value":"YULG2JI2LLLO","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"YULG2JI2LLLOGAI4","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"YULG2JI2","created_at":"2026-05-18T12:27:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:YULG2JI2LLLOGAI4DMPQRQ5JRN","target":"record","payload":{"canonical_record":{"source":{"id":"1212.4553","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2012-12-19T01:44:10Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"2d442dd7a10a4cd6e483d7a0cfcd8b51d8313ac43308c1c8cc86cfecd1d7b4c5","abstract_canon_sha256":"729fbc70cd3bface77d88341ed4bdc7f1121aee14f2058566bdb293579e21270"},"schema_version":"1.0"},"canonical_sha256":"c5166d251a5ad6e3011c1b1f08c3a98b6f5d7fbf83d9c9e7614b636b9de6e67a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:36:17.719559Z","signature_b64":"1w8V9TVWwTnjzv0d4IkumXIcl2xsqReGgdz4hgpQeMqYzstmFjbuhD0k0VhYgPkramHPP7unKEkA0T2IrHAVBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c5166d251a5ad6e3011c1b1f08c3a98b6f5d7fbf83d9c9e7614b636b9de6e67a","last_reissued_at":"2026-05-18T03:36:17.718909Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:36:17.718909Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1212.4553","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:36:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"99aMPxuh/z6mEC5QiKyhbOWAVFE7l+8qK1ThBx0XZ9ka3wJNfzeXOeZ9TzczfusTrYHTwnKkuSvqEtfzXBYHDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T12:18:14.806970Z"},"content_sha256":"852669d0893d28ae315c5521a1ffa7e8db28582f9ed754d839e1d19b616acc4f","schema_version":"1.0","event_id":"sha256:852669d0893d28ae315c5521a1ffa7e8db28582f9ed754d839e1d19b616acc4f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:YULG2JI2LLLOGAI4DMPQRQ5JRN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Five-dimensional heterotic black holes and its dual IR-CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"physics.gen-ph","authors_text":"Hossein Yavartanoo","submitted_at":"2012-12-19T01:44:10Z","abstract_excerpt":"We analyze the possible dynamical emergence of IR conformal field theory describing the low- energy excitations of near-extremal black holes in five-dimensional compactification of heterotic strings. We find that, by tuning the mass and charges in such a way that the extremal black holes have a classically vanishing horizon area, the near-horizon develops an AdS3 throat and when we combine the low-energy limit with vanishing Newton coupling constant, the system has a dual conformal field theory description. We compare our results with c-extremization and the Kerr/CFT predictions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.4553","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:36:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uctaCjjEdRwG4JHnuHZLe2c66+C3Oy3diHsBE6O5hLs8pTMhSDMmSnDQHfNp+3C1Mz/+hs99b1cSP1xH7UFlAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T12:18:14.807357Z"},"content_sha256":"9d2cd9ae2b3a6417d8686b8ac31c4809eaa85cb92f0624867966820ef0b39f7e","schema_version":"1.0","event_id":"sha256:9d2cd9ae2b3a6417d8686b8ac31c4809eaa85cb92f0624867966820ef0b39f7e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YULG2JI2LLLOGAI4DMPQRQ5JRN/bundle.json","state_url":"https://pith.science/pith/YULG2JI2LLLOGAI4DMPQRQ5JRN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YULG2JI2LLLOGAI4DMPQRQ5JRN/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-25T12:18:14Z","links":{"resolver":"https://pith.science/pith/YULG2JI2LLLOGAI4DMPQRQ5JRN","bundle":"https://pith.science/pith/YULG2JI2LLLOGAI4DMPQRQ5JRN/bundle.json","state":"https://pith.science/pith/YULG2JI2LLLOGAI4DMPQRQ5JRN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YULG2JI2LLLOGAI4DMPQRQ5JRN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:YULG2JI2LLLOGAI4DMPQRQ5JRN","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"729fbc70cd3bface77d88341ed4bdc7f1121aee14f2058566bdb293579e21270","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2012-12-19T01:44:10Z","title_canon_sha256":"2d442dd7a10a4cd6e483d7a0cfcd8b51d8313ac43308c1c8cc86cfecd1d7b4c5"},"schema_version":"1.0","source":{"id":"1212.4553","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.4553","created_at":"2026-05-18T03:36:17Z"},{"alias_kind":"arxiv_version","alias_value":"1212.4553v3","created_at":"2026-05-18T03:36:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.4553","created_at":"2026-05-18T03:36:17Z"},{"alias_kind":"pith_short_12","alias_value":"YULG2JI2LLLO","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"YULG2JI2LLLOGAI4","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"YULG2JI2","created_at":"2026-05-18T12:27:30Z"}],"graph_snapshots":[{"event_id":"sha256:9d2cd9ae2b3a6417d8686b8ac31c4809eaa85cb92f0624867966820ef0b39f7e","target":"graph","created_at":"2026-05-18T03:36:17Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We analyze the possible dynamical emergence of IR conformal field theory describing the low- energy excitations of near-extremal black holes in five-dimensional compactification of heterotic strings. We find that, by tuning the mass and charges in such a way that the extremal black holes have a classically vanishing horizon area, the near-horizon develops an AdS3 throat and when we combine the low-energy limit with vanishing Newton coupling constant, the system has a dual conformal field theory description. We compare our results with c-extremization and the Kerr/CFT predictions.","authors_text":"Hossein Yavartanoo","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2012-12-19T01:44:10Z","title":"Five-dimensional heterotic black holes and its dual IR-CFT"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.4553","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:852669d0893d28ae315c5521a1ffa7e8db28582f9ed754d839e1d19b616acc4f","target":"record","created_at":"2026-05-18T03:36:17Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"729fbc70cd3bface77d88341ed4bdc7f1121aee14f2058566bdb293579e21270","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2012-12-19T01:44:10Z","title_canon_sha256":"2d442dd7a10a4cd6e483d7a0cfcd8b51d8313ac43308c1c8cc86cfecd1d7b4c5"},"schema_version":"1.0","source":{"id":"1212.4553","kind":"arxiv","version":3}},"canonical_sha256":"c5166d251a5ad6e3011c1b1f08c3a98b6f5d7fbf83d9c9e7614b636b9de6e67a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c5166d251a5ad6e3011c1b1f08c3a98b6f5d7fbf83d9c9e7614b636b9de6e67a","first_computed_at":"2026-05-18T03:36:17.718909Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:36:17.718909Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1w8V9TVWwTnjzv0d4IkumXIcl2xsqReGgdz4hgpQeMqYzstmFjbuhD0k0VhYgPkramHPP7unKEkA0T2IrHAVBg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:36:17.719559Z","signed_message":"canonical_sha256_bytes"},"source_id":"1212.4553","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:852669d0893d28ae315c5521a1ffa7e8db28582f9ed754d839e1d19b616acc4f","sha256:9d2cd9ae2b3a6417d8686b8ac31c4809eaa85cb92f0624867966820ef0b39f7e"],"state_sha256":"7ebbd800ea000f5f7ed85973c9517aa6756e39af80a5e683cbf7f82ab4b5d5e9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0BOntV9/EvFMsFSeMzuCcOR7A4oOn37Ipxl6qrr0PqOEXeIpOkbhF5DkqvgaD51da/4NhPbIEE2XE/MjmkjqDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T12:18:14.810491Z","bundle_sha256":"509b08c93160f64962af1c231d0d2f4f1e44e1a4b91f1967b8458b90088335ba"}}