{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:4IB7JP3GOKR6JSXWMIRGS3ULYB","short_pith_number":"pith:4IB7JP3G","schema_version":"1.0","canonical_sha256":"e203f4bf6672a3e4caf66222696e8bc07273f4c9f12b05bb978a448dd8789ada","source":{"kind":"arxiv","id":"1803.03633","version":2},"attestation_state":"computed","paper":{"title":"Holographic second laws of black hole thermodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","quant-ph"],"primary_cat":"hep-th","authors_text":"Alice Bernamonti, Federico Galli, Jonathan Oppenheim, Robert C. Myers","submitted_at":"2018-03-09T18:46:29Z","abstract_excerpt":"Recently, it has been shown that for out-of-equilibrium systems, there are additional constraints on thermodynamical evolution besides the ordinary second law. These form a new family of second laws of thermodynamics, which are equivalent to the monotonicity of quantum R\\'enyi divergences. In black hole thermodynamics, the usual second law is manifest as the area increase theorem. Hence one may ask if these additional laws imply new restrictions for gravitational dynamics, such as for out-of-equilibrium black holes? Inspired by this question, we study these constraints within the AdS/CFT corre"},"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":"1803.03633","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-09T18:46:29Z","cross_cats_sorted":["gr-qc","quant-ph"],"title_canon_sha256":"1db379cf7c603200e1ea0c03447635bb93aea94e8cd670c91442b3ef3eca201a","abstract_canon_sha256":"4c26ff4e3782919d32a1048b9bc28658827ccf4be3ff5ca15ea3683255bfd9b1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:03:49.408381Z","signature_b64":"rHisE9cxsEAYwYJp0JerkMTEq56JSc+2EfF2btiqdRk8hzOyVV5/ZwQPNSmZKXlI6tg6w692Cf9e5vXYLVgqAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e203f4bf6672a3e4caf66222696e8bc07273f4c9f12b05bb978a448dd8789ada","last_reissued_at":"2026-05-18T00:03:49.407867Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:03:49.407867Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic second laws of black hole thermodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","quant-ph"],"primary_cat":"hep-th","authors_text":"Alice Bernamonti, Federico Galli, Jonathan Oppenheim, Robert C. Myers","submitted_at":"2018-03-09T18:46:29Z","abstract_excerpt":"Recently, it has been shown that for out-of-equilibrium systems, there are additional constraints on thermodynamical evolution besides the ordinary second law. These form a new family of second laws of thermodynamics, which are equivalent to the monotonicity of quantum R\\'enyi divergences. In black hole thermodynamics, the usual second law is manifest as the area increase theorem. Hence one may ask if these additional laws imply new restrictions for gravitational dynamics, such as for out-of-equilibrium black holes? Inspired by this question, we study these constraints within the AdS/CFT corre"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.03633","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":""},"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":"1803.03633","created_at":"2026-05-18T00:03:49.407952+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.03633v2","created_at":"2026-05-18T00:03:49.407952+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.03633","created_at":"2026-05-18T00:03:49.407952+00:00"},{"alias_kind":"pith_short_12","alias_value":"4IB7JP3GOKR6","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_16","alias_value":"4IB7JP3GOKR6JSXW","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_8","alias_value":"4IB7JP3G","created_at":"2026-05-18T12:32:05.422762+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4IB7JP3GOKR6JSXWMIRGS3ULYB","json":"https://pith.science/pith/4IB7JP3GOKR6JSXWMIRGS3ULYB.json","graph_json":"https://pith.science/api/pith-number/4IB7JP3GOKR6JSXWMIRGS3ULYB/graph.json","events_json":"https://pith.science/api/pith-number/4IB7JP3GOKR6JSXWMIRGS3ULYB/events.json","paper":"https://pith.science/paper/4IB7JP3G"},"agent_actions":{"view_html":"https://pith.science/pith/4IB7JP3GOKR6JSXWMIRGS3ULYB","download_json":"https://pith.science/pith/4IB7JP3GOKR6JSXWMIRGS3ULYB.json","view_paper":"https://pith.science/paper/4IB7JP3G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.03633&json=true","fetch_graph":"https://pith.science/api/pith-number/4IB7JP3GOKR6JSXWMIRGS3ULYB/graph.json","fetch_events":"https://pith.science/api/pith-number/4IB7JP3GOKR6JSXWMIRGS3ULYB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4IB7JP3GOKR6JSXWMIRGS3ULYB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4IB7JP3GOKR6JSXWMIRGS3ULYB/action/storage_attestation","attest_author":"https://pith.science/pith/4IB7JP3GOKR6JSXWMIRGS3ULYB/action/author_attestation","sign_citation":"https://pith.science/pith/4IB7JP3GOKR6JSXWMIRGS3ULYB/action/citation_signature","submit_replication":"https://pith.science/pith/4IB7JP3GOKR6JSXWMIRGS3ULYB/action/replication_record"}},"created_at":"2026-05-18T00:03:49.407952+00:00","updated_at":"2026-05-18T00:03:49.407952+00:00"}