{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:Q425F2C76DN2EFSSVB75SPXDOT","short_pith_number":"pith:Q425F2C7","schema_version":"1.0","canonical_sha256":"8735d2e85ff0dba21652a87fd93ee374ef7ee1f27061427abe31be0db022fdc9","source":{"kind":"arxiv","id":"1511.02288","version":2},"attestation_state":"computed","paper":{"title":"Thermodynamic law from the entanglement entropy bound","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chanyong Park","submitted_at":"2015-11-07T02:55:29Z","abstract_excerpt":"From black hole thermodynamics, the Bekenstein bound has been proposed as a universal thermal entropy bound. It has been further generalized to an entanglement entropy bound which is valid even in a quantum system. In a quantumly entangled system, the non-negativity of the relative entropy leads to the entanglement entropy bound. When the entanglement entropy bound is saturated, a quantum system satisfies the thermodynamics-like law with an appropriately defined entanglement temperature. We show that the saturation of the entanglement entropy bound accounts for a universal feature of the entan"},"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":"1511.02288","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-11-07T02:55:29Z","cross_cats_sorted":[],"title_canon_sha256":"a9994a777359715983939762913d5eb2327b35c06eb22310e7c235cb27831729","abstract_canon_sha256":"7522e6b6be340e2c6aa9e87aa29e3c96193bb501a1afd53d32448c9fc2b8d0c3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:45.743954Z","signature_b64":"kiWICmF1kIcpiy5axgIRvGbxOMD4ovij/v3AqXXQ3rs9caQgua+g5gMGR6D4mD2842+aezl0TXFXwKpk0CGLAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8735d2e85ff0dba21652a87fd93ee374ef7ee1f27061427abe31be0db022fdc9","last_reissued_at":"2026-05-18T01:16:45.743205Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:45.743205Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamic law from the entanglement entropy bound","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chanyong Park","submitted_at":"2015-11-07T02:55:29Z","abstract_excerpt":"From black hole thermodynamics, the Bekenstein bound has been proposed as a universal thermal entropy bound. It has been further generalized to an entanglement entropy bound which is valid even in a quantum system. In a quantumly entangled system, the non-negativity of the relative entropy leads to the entanglement entropy bound. When the entanglement entropy bound is saturated, a quantum system satisfies the thermodynamics-like law with an appropriately defined entanglement temperature. We show that the saturation of the entanglement entropy bound accounts for a universal feature of the entan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.02288","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":"1511.02288","created_at":"2026-05-18T01:16:45.743336+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.02288v2","created_at":"2026-05-18T01:16:45.743336+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.02288","created_at":"2026-05-18T01:16:45.743336+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q425F2C76DN2","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q425F2C76DN2EFSS","created_at":"2026-05-18T12:29:37.295048+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q425F2C7","created_at":"2026-05-18T12:29:37.295048+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.15736","citing_title":"Heavy holographic correlators in defect conformal field theories","ref_index":47,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Q425F2C76DN2EFSSVB75SPXDOT","json":"https://pith.science/pith/Q425F2C76DN2EFSSVB75SPXDOT.json","graph_json":"https://pith.science/api/pith-number/Q425F2C76DN2EFSSVB75SPXDOT/graph.json","events_json":"https://pith.science/api/pith-number/Q425F2C76DN2EFSSVB75SPXDOT/events.json","paper":"https://pith.science/paper/Q425F2C7"},"agent_actions":{"view_html":"https://pith.science/pith/Q425F2C76DN2EFSSVB75SPXDOT","download_json":"https://pith.science/pith/Q425F2C76DN2EFSSVB75SPXDOT.json","view_paper":"https://pith.science/paper/Q425F2C7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.02288&json=true","fetch_graph":"https://pith.science/api/pith-number/Q425F2C76DN2EFSSVB75SPXDOT/graph.json","fetch_events":"https://pith.science/api/pith-number/Q425F2C76DN2EFSSVB75SPXDOT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q425F2C76DN2EFSSVB75SPXDOT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q425F2C76DN2EFSSVB75SPXDOT/action/storage_attestation","attest_author":"https://pith.science/pith/Q425F2C76DN2EFSSVB75SPXDOT/action/author_attestation","sign_citation":"https://pith.science/pith/Q425F2C76DN2EFSSVB75SPXDOT/action/citation_signature","submit_replication":"https://pith.science/pith/Q425F2C76DN2EFSSVB75SPXDOT/action/replication_record"}},"created_at":"2026-05-18T01:16:45.743336+00:00","updated_at":"2026-05-18T01:16:45.743336+00:00"}