{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:HQAJFPM477CRE4KPAYXGS54CIQ","short_pith_number":"pith:HQAJFPM4","schema_version":"1.0","canonical_sha256":"3c0092bd9cffc512714f062e6977824421d87467d6b64459033d6b0ae2576f36","source":{"kind":"arxiv","id":"1910.08061","version":1},"attestation_state":"computed","paper":{"title":"Entropy Counting from Schwarzschild/CFT and Soft Hair","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Artem Averin","submitted_at":"2019-10-17T17:47:10Z","abstract_excerpt":"We revisit Carlip's approach to entropy counting. This analysis reemerged in a recently obtained Schwarzschild/CFT-correspondence as Sugawara-construction of a 2D stress-tensor. Here, for the example of a Schwarzschild black hole, we show how to single out diffeomorphisms forming in contrast to Carlip's analysis the full 2D local conformal algebra. We provide arguments, why their Hamiltonian generators are expected to be the symmetry generators of a possible conformal field theory describing the part of phase space responsible for black hole microstates. Then, we can infer central charges and "},"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":"1910.08061","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-10-17T17:47:10Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"8482ee54b179efd199f92f97fa80b19f493b8421c6c8af6b981d74ecc8f61201","abstract_canon_sha256":"6b75c36c1a34dc42284e0c5d74f21339e1e477625f3ee448c1a3bb4934503471"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:43:38.774378Z","signature_b64":"d3hoAuOZd3cEGr/ktL60Pbmvw5B6C4tRxiV33UEQCzziCsBxznh9rCJ/UYEQg3jfFyj9oaVoKKSRSZSPQgijCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c0092bd9cffc512714f062e6977824421d87467d6b64459033d6b0ae2576f36","last_reissued_at":"2026-07-05T00:43:38.773907Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:43:38.773907Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Entropy Counting from Schwarzschild/CFT and Soft Hair","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Artem Averin","submitted_at":"2019-10-17T17:47:10Z","abstract_excerpt":"We revisit Carlip's approach to entropy counting. This analysis reemerged in a recently obtained Schwarzschild/CFT-correspondence as Sugawara-construction of a 2D stress-tensor. Here, for the example of a Schwarzschild black hole, we show how to single out diffeomorphisms forming in contrast to Carlip's analysis the full 2D local conformal algebra. We provide arguments, why their Hamiltonian generators are expected to be the symmetry generators of a possible conformal field theory describing the part of phase space responsible for black hole microstates. Then, we can infer central charges and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1910.08061","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1910.08061/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":"1910.08061","created_at":"2026-07-05T00:43:38.773964+00:00"},{"alias_kind":"arxiv_version","alias_value":"1910.08061v1","created_at":"2026-07-05T00:43:38.773964+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1910.08061","created_at":"2026-07-05T00:43:38.773964+00:00"},{"alias_kind":"pith_short_12","alias_value":"HQAJFPM477CR","created_at":"2026-07-05T00:43:38.773964+00:00"},{"alias_kind":"pith_short_16","alias_value":"HQAJFPM477CRE4KP","created_at":"2026-07-05T00:43:38.773964+00:00"},{"alias_kind":"pith_short_8","alias_value":"HQAJFPM4","created_at":"2026-07-05T00:43:38.773964+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.02470","citing_title":"Formulation and Proof of the Gravitational Entropy Bound","ref_index":6,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HQAJFPM477CRE4KPAYXGS54CIQ","json":"https://pith.science/pith/HQAJFPM477CRE4KPAYXGS54CIQ.json","graph_json":"https://pith.science/api/pith-number/HQAJFPM477CRE4KPAYXGS54CIQ/graph.json","events_json":"https://pith.science/api/pith-number/HQAJFPM477CRE4KPAYXGS54CIQ/events.json","paper":"https://pith.science/paper/HQAJFPM4"},"agent_actions":{"view_html":"https://pith.science/pith/HQAJFPM477CRE4KPAYXGS54CIQ","download_json":"https://pith.science/pith/HQAJFPM477CRE4KPAYXGS54CIQ.json","view_paper":"https://pith.science/paper/HQAJFPM4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1910.08061&json=true","fetch_graph":"https://pith.science/api/pith-number/HQAJFPM477CRE4KPAYXGS54CIQ/graph.json","fetch_events":"https://pith.science/api/pith-number/HQAJFPM477CRE4KPAYXGS54CIQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HQAJFPM477CRE4KPAYXGS54CIQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HQAJFPM477CRE4KPAYXGS54CIQ/action/storage_attestation","attest_author":"https://pith.science/pith/HQAJFPM477CRE4KPAYXGS54CIQ/action/author_attestation","sign_citation":"https://pith.science/pith/HQAJFPM477CRE4KPAYXGS54CIQ/action/citation_signature","submit_replication":"https://pith.science/pith/HQAJFPM477CRE4KPAYXGS54CIQ/action/replication_record"}},"created_at":"2026-07-05T00:43:38.773964+00:00","updated_at":"2026-07-05T00:43:38.773964+00:00"}