{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:3MKWZ3ECFMCKJ6EJECREVO2KNB","short_pith_number":"pith:3MKWZ3EC","schema_version":"1.0","canonical_sha256":"db156cec822b04a4f88920a24abb4a687c48e291e12367072bf2f8bfdfa6d899","source":{"kind":"arxiv","id":"1008.3027","version":2},"attestation_state":"computed","paper":{"title":"Evolution of Holographic Entanglement Entropy after Thermal and Electromagnetic Quenches","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Clifford V. Johnson, Tameem Albash","submitted_at":"2010-08-18T06:27:34Z","abstract_excerpt":"We study the evolution and scaling of the entanglement entropy after two types of quenches for a 2+1 field theory, using holographic techniques. We study a thermal quench, dual to the addition of a shell of uncharged matter to four dimensional Anti-de Sitter (AdS_4) spacetime, and study the subsequent formation of a Schwarzschild black hole. We also study an electromagnetic quench, dual to the addition of a shell of charged sources to AdS_4, following the subsequent formation of an extremal dyonic black hole. In these backgrounds we consider the entanglement entropy of two types of geometries,"},"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":"1008.3027","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-08-18T06:27:34Z","cross_cats_sorted":[],"title_canon_sha256":"8c866141d489aec94036e3f5cba5482a20314d213732f0b33b5089afb4c15c25","abstract_canon_sha256":"e0fd953ab133258cfd4b14721ca0c8e576934b97bf29e8cbf58bcc50f1c06146"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:50.325599Z","signature_b64":"0yQLJoPUzhdg0wLJYeLHzGVuGfXyyiDBbEUrXHilZE1Zz6+wAug1FcFb1f/9CbB434ZvXmU4MMBTMbdBZ4X8Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"db156cec822b04a4f88920a24abb4a687c48e291e12367072bf2f8bfdfa6d899","last_reissued_at":"2026-05-18T04:15:50.325118Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:50.325118Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Evolution of Holographic Entanglement Entropy after Thermal and Electromagnetic Quenches","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Clifford V. Johnson, Tameem Albash","submitted_at":"2010-08-18T06:27:34Z","abstract_excerpt":"We study the evolution and scaling of the entanglement entropy after two types of quenches for a 2+1 field theory, using holographic techniques. We study a thermal quench, dual to the addition of a shell of uncharged matter to four dimensional Anti-de Sitter (AdS_4) spacetime, and study the subsequent formation of a Schwarzschild black hole. We also study an electromagnetic quench, dual to the addition of a shell of charged sources to AdS_4, following the subsequent formation of an extremal dyonic black hole. In these backgrounds we consider the entanglement entropy of two types of geometries,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.3027","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":"1008.3027","created_at":"2026-05-18T04:15:50.325188+00:00"},{"alias_kind":"arxiv_version","alias_value":"1008.3027v2","created_at":"2026-05-18T04:15:50.325188+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.3027","created_at":"2026-05-18T04:15:50.325188+00:00"},{"alias_kind":"pith_short_12","alias_value":"3MKWZ3ECFMCK","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_16","alias_value":"3MKWZ3ECFMCKJ6EJ","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_8","alias_value":"3MKWZ3EC","created_at":"2026-05-18T12:26:03.138858+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/3MKWZ3ECFMCKJ6EJECREVO2KNB","json":"https://pith.science/pith/3MKWZ3ECFMCKJ6EJECREVO2KNB.json","graph_json":"https://pith.science/api/pith-number/3MKWZ3ECFMCKJ6EJECREVO2KNB/graph.json","events_json":"https://pith.science/api/pith-number/3MKWZ3ECFMCKJ6EJECREVO2KNB/events.json","paper":"https://pith.science/paper/3MKWZ3EC"},"agent_actions":{"view_html":"https://pith.science/pith/3MKWZ3ECFMCKJ6EJECREVO2KNB","download_json":"https://pith.science/pith/3MKWZ3ECFMCKJ6EJECREVO2KNB.json","view_paper":"https://pith.science/paper/3MKWZ3EC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1008.3027&json=true","fetch_graph":"https://pith.science/api/pith-number/3MKWZ3ECFMCKJ6EJECREVO2KNB/graph.json","fetch_events":"https://pith.science/api/pith-number/3MKWZ3ECFMCKJ6EJECREVO2KNB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3MKWZ3ECFMCKJ6EJECREVO2KNB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3MKWZ3ECFMCKJ6EJECREVO2KNB/action/storage_attestation","attest_author":"https://pith.science/pith/3MKWZ3ECFMCKJ6EJECREVO2KNB/action/author_attestation","sign_citation":"https://pith.science/pith/3MKWZ3ECFMCKJ6EJECREVO2KNB/action/citation_signature","submit_replication":"https://pith.science/pith/3MKWZ3ECFMCKJ6EJECREVO2KNB/action/replication_record"}},"created_at":"2026-05-18T04:15:50.325188+00:00","updated_at":"2026-05-18T04:15:50.325188+00:00"}