{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:SQWUVMXTKWUHVKQSESUBBUYQVG","short_pith_number":"pith:SQWUVMXT","schema_version":"1.0","canonical_sha256":"942d4ab2f355a87aaa1224a810d310a9a4e8c8719a80b162d2d485e23d6500d4","source":{"kind":"arxiv","id":"2607.15276","version":1},"attestation_state":"computed","paper":{"title":"Locality of deep thermalisation through the lens of entanglement teleportation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech","hep-th"],"primary_cat":"quant-ph","authors_text":"Alan Sherry, Saptarshi Mandal, Sthitadhi Roy","submitted_at":"2026-07-16T17:59:16Z","abstract_excerpt":"Deep thermalisation characterises the emergence of universal quantum state ensembles on subsystems due to projective measurements on their complement. We study the notion of locality, or lack thereof, in this phenomenon by considering a subsystem partitioned into two disjoint subregions which remain causally disconnected at all times under unitary dynamics. We show that the onset of deep thermalisation in this geometry is fundamentally bounded by measurement-induced entanglement teleportation between the subregions. While measurements on the environment generate entanglement across the disconn"},"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":"2607.15276","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-07-16T17:59:16Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech","hep-th"],"title_canon_sha256":"05b0685fdd2791bda4fc04496c0184d94a4d976325faabe8565bb7beef03164c","abstract_canon_sha256":"20ff7b034a305533a5f94191677f2f450b50e26e8b41c145d6e089503f5488f5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-17T01:22:18.231101Z","signature_b64":"XFdQjIUlBVRAD7Vc/mnxnKSRu2Xp1lGMqtQLt/LognIAqm6o1XXOgAubGK08y8L3awuioCWetX2Y8JfR7A2UAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"942d4ab2f355a87aaa1224a810d310a9a4e8c8719a80b162d2d485e23d6500d4","last_reissued_at":"2026-07-17T01:22:18.230233Z","signature_status":"signed_v1","first_computed_at":"2026-07-17T01:22:18.230233Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Locality of deep thermalisation through the lens of entanglement teleportation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech","hep-th"],"primary_cat":"quant-ph","authors_text":"Alan Sherry, Saptarshi Mandal, Sthitadhi Roy","submitted_at":"2026-07-16T17:59:16Z","abstract_excerpt":"Deep thermalisation characterises the emergence of universal quantum state ensembles on subsystems due to projective measurements on their complement. We study the notion of locality, or lack thereof, in this phenomenon by considering a subsystem partitioned into two disjoint subregions which remain causally disconnected at all times under unitary dynamics. We show that the onset of deep thermalisation in this geometry is fundamentally bounded by measurement-induced entanglement teleportation between the subregions. While measurements on the environment generate entanglement across the disconn"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.15276","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/2607.15276/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":"2607.15276","created_at":"2026-07-17T01:22:18.230690+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.15276v1","created_at":"2026-07-17T01:22:18.230690+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.15276","created_at":"2026-07-17T01:22:18.230690+00:00"},{"alias_kind":"pith_short_12","alias_value":"SQWUVMXTKWUH","created_at":"2026-07-17T01:22:18.230690+00:00"},{"alias_kind":"pith_short_16","alias_value":"SQWUVMXTKWUHVKQS","created_at":"2026-07-17T01:22:18.230690+00:00"},{"alias_kind":"pith_short_8","alias_value":"SQWUVMXT","created_at":"2026-07-17T01:22:18.230690+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/SQWUVMXTKWUHVKQSESUBBUYQVG","json":"https://pith.science/pith/SQWUVMXTKWUHVKQSESUBBUYQVG.json","graph_json":"https://pith.science/api/pith-number/SQWUVMXTKWUHVKQSESUBBUYQVG/graph.json","events_json":"https://pith.science/api/pith-number/SQWUVMXTKWUHVKQSESUBBUYQVG/events.json","paper":"https://pith.science/paper/SQWUVMXT"},"agent_actions":{"view_html":"https://pith.science/pith/SQWUVMXTKWUHVKQSESUBBUYQVG","download_json":"https://pith.science/pith/SQWUVMXTKWUHVKQSESUBBUYQVG.json","view_paper":"https://pith.science/paper/SQWUVMXT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.15276&json=true","fetch_graph":"https://pith.science/api/pith-number/SQWUVMXTKWUHVKQSESUBBUYQVG/graph.json","fetch_events":"https://pith.science/api/pith-number/SQWUVMXTKWUHVKQSESUBBUYQVG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SQWUVMXTKWUHVKQSESUBBUYQVG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SQWUVMXTKWUHVKQSESUBBUYQVG/action/storage_attestation","attest_author":"https://pith.science/pith/SQWUVMXTKWUHVKQSESUBBUYQVG/action/author_attestation","sign_citation":"https://pith.science/pith/SQWUVMXTKWUHVKQSESUBBUYQVG/action/citation_signature","submit_replication":"https://pith.science/pith/SQWUVMXTKWUHVKQSESUBBUYQVG/action/replication_record"}},"created_at":"2026-07-17T01:22:18.230690+00:00","updated_at":"2026-07-17T01:22:18.230690+00:00"}