{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:5P4H4WOKKRXIK3HCUGQDETHT25","short_pith_number":"pith:5P4H4WOK","canonical_record":{"source":{"id":"1711.01740","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-06T06:23:31Z","cross_cats_sorted":["cond-mat.quant-gas","nucl-th"],"title_canon_sha256":"149a9a81aa7405e7530d7bf2061c629d8a867f2ba0183b0b5474cbf9c32f560a","abstract_canon_sha256":"478625ff703f76f2b5e82bf090ff0ab3e79e70b2e48fe3f29feeb2a24ca4e6ee"},"schema_version":"1.0"},"canonical_sha256":"ebf87e59ca546e856ce2a1a0324cf3d77440405b1df9dae0a94dcc2b0e508511","source":{"kind":"arxiv","id":"1711.01740","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.01740","created_at":"2026-05-18T00:23:08Z"},{"alias_kind":"arxiv_version","alias_value":"1711.01740v2","created_at":"2026-05-18T00:23:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.01740","created_at":"2026-05-18T00:23:08Z"},{"alias_kind":"pith_short_12","alias_value":"5P4H4WOKKRXI","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_16","alias_value":"5P4H4WOKKRXIK3HC","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_8","alias_value":"5P4H4WOK","created_at":"2026-05-18T12:31:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:5P4H4WOKKRXIK3HCUGQDETHT25","target":"record","payload":{"canonical_record":{"source":{"id":"1711.01740","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-06T06:23:31Z","cross_cats_sorted":["cond-mat.quant-gas","nucl-th"],"title_canon_sha256":"149a9a81aa7405e7530d7bf2061c629d8a867f2ba0183b0b5474cbf9c32f560a","abstract_canon_sha256":"478625ff703f76f2b5e82bf090ff0ab3e79e70b2e48fe3f29feeb2a24ca4e6ee"},"schema_version":"1.0"},"canonical_sha256":"ebf87e59ca546e856ce2a1a0324cf3d77440405b1df9dae0a94dcc2b0e508511","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:23:08.247503Z","signature_b64":"P6BHLfWLtLOIBWA1zqfDI8Rg6yKT2YbmkZPJE33+kM72KAOYMnKWTQH90+o7FalKfXFJSQtS3nnih7VTBqldBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ebf87e59ca546e856ce2a1a0324cf3d77440405b1df9dae0a94dcc2b0e508511","last_reissued_at":"2026-05-18T00:23:08.246801Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:23:08.246801Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.01740","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:23:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xrkkWsordRG25PnAHTfvB84LX6HGa0Gfpiz5Fy+txEsszf8T0lNVwJOJqNIoLOivIXoxzCaMu40MypKgeEznDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:37:01.378223Z"},"content_sha256":"426602d51147bd70fb4c686143ed099c28fdfae4214475ef46ee045a23a0d901","schema_version":"1.0","event_id":"sha256:426602d51147bd70fb4c686143ed099c28fdfae4214475ef46ee045a23a0d901"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:5P4H4WOKKRXIK3HCUGQDETHT25","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Semiclassical theory of strong localization for quantum thermalization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","nucl-th"],"primary_cat":"quant-ph","authors_text":"Amichay Vardi, Christine Khripkov, Doron Cohen","submitted_at":"2017-11-06T06:23:31Z","abstract_excerpt":"We introduce a semiclassical theory for strong localization that may arise in the context of many-body thermalization. As a minimal model for thermalization we consider a few-site Bose-Hubbard model consisting of two weakly interacting subsystems that can exchange particles. The occupation of a subsystem ($x$) satisfies in the classical treatment a Fokker-Planck equation with a diffusion coefficient $D(x)$. We demonstrate that it is possible to deduce from the classical description a quantum breaktime $t^*$, and hence the manifestations of a strong localization effect. For this purpose it is e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.01740","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:23:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2iiGHGnj0LRebrCsmRLr9rWzyyFj5JI4BScLEOhnK87w7ARUxYCV2O2/zD93cqRZ1rKMvW8oc/ykNyjRy7WjDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:37:01.378872Z"},"content_sha256":"3a60acdf2e886b44597e2eeb4a6fbdaae5e3721a74fdd9d002256e50855406b9","schema_version":"1.0","event_id":"sha256:3a60acdf2e886b44597e2eeb4a6fbdaae5e3721a74fdd9d002256e50855406b9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5P4H4WOKKRXIK3HCUGQDETHT25/bundle.json","state_url":"https://pith.science/pith/5P4H4WOKKRXIK3HCUGQDETHT25/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5P4H4WOKKRXIK3HCUGQDETHT25/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-26T21:37:01Z","links":{"resolver":"https://pith.science/pith/5P4H4WOKKRXIK3HCUGQDETHT25","bundle":"https://pith.science/pith/5P4H4WOKKRXIK3HCUGQDETHT25/bundle.json","state":"https://pith.science/pith/5P4H4WOKKRXIK3HCUGQDETHT25/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5P4H4WOKKRXIK3HCUGQDETHT25/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:5P4H4WOKKRXIK3HCUGQDETHT25","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"478625ff703f76f2b5e82bf090ff0ab3e79e70b2e48fe3f29feeb2a24ca4e6ee","cross_cats_sorted":["cond-mat.quant-gas","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-06T06:23:31Z","title_canon_sha256":"149a9a81aa7405e7530d7bf2061c629d8a867f2ba0183b0b5474cbf9c32f560a"},"schema_version":"1.0","source":{"id":"1711.01740","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.01740","created_at":"2026-05-18T00:23:08Z"},{"alias_kind":"arxiv_version","alias_value":"1711.01740v2","created_at":"2026-05-18T00:23:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.01740","created_at":"2026-05-18T00:23:08Z"},{"alias_kind":"pith_short_12","alias_value":"5P4H4WOKKRXI","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_16","alias_value":"5P4H4WOKKRXIK3HC","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_8","alias_value":"5P4H4WOK","created_at":"2026-05-18T12:31:00Z"}],"graph_snapshots":[{"event_id":"sha256:3a60acdf2e886b44597e2eeb4a6fbdaae5e3721a74fdd9d002256e50855406b9","target":"graph","created_at":"2026-05-18T00:23:08Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We introduce a semiclassical theory for strong localization that may arise in the context of many-body thermalization. As a minimal model for thermalization we consider a few-site Bose-Hubbard model consisting of two weakly interacting subsystems that can exchange particles. The occupation of a subsystem ($x$) satisfies in the classical treatment a Fokker-Planck equation with a diffusion coefficient $D(x)$. We demonstrate that it is possible to deduce from the classical description a quantum breaktime $t^*$, and hence the manifestations of a strong localization effect. For this purpose it is e","authors_text":"Amichay Vardi, Christine Khripkov, Doron Cohen","cross_cats":["cond-mat.quant-gas","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-06T06:23:31Z","title":"Semiclassical theory of strong localization for quantum thermalization"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.01740","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:426602d51147bd70fb4c686143ed099c28fdfae4214475ef46ee045a23a0d901","target":"record","created_at":"2026-05-18T00:23:08Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"478625ff703f76f2b5e82bf090ff0ab3e79e70b2e48fe3f29feeb2a24ca4e6ee","cross_cats_sorted":["cond-mat.quant-gas","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-06T06:23:31Z","title_canon_sha256":"149a9a81aa7405e7530d7bf2061c629d8a867f2ba0183b0b5474cbf9c32f560a"},"schema_version":"1.0","source":{"id":"1711.01740","kind":"arxiv","version":2}},"canonical_sha256":"ebf87e59ca546e856ce2a1a0324cf3d77440405b1df9dae0a94dcc2b0e508511","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ebf87e59ca546e856ce2a1a0324cf3d77440405b1df9dae0a94dcc2b0e508511","first_computed_at":"2026-05-18T00:23:08.246801Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:23:08.246801Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"P6BHLfWLtLOIBWA1zqfDI8Rg6yKT2YbmkZPJE33+kM72KAOYMnKWTQH90+o7FalKfXFJSQtS3nnih7VTBqldBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:23:08.247503Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.01740","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:426602d51147bd70fb4c686143ed099c28fdfae4214475ef46ee045a23a0d901","sha256:3a60acdf2e886b44597e2eeb4a6fbdaae5e3721a74fdd9d002256e50855406b9"],"state_sha256":"7c74648e87a9e5268946be8f2819bac2589c1a08072b4b16b0c79dca05f4edd4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KVqn5U9kGDk3OIgzVyUrZP5fl9ZD3137jdzobkluoKiLtm5AGVN0KThlssjEx4zE/nJqp+Kwa71sG79dXUtvDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T21:37:01.381366Z","bundle_sha256":"dd87bd3fe6614f3874597f902a32750e0eb6895a2b7a20a6988c9a491f378263"}}