{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:VSTVRFDVDXFDHA5HFQZQNVWXK6","short_pith_number":"pith:VSTVRFDV","canonical_record":{"source":{"id":"2408.15325","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-08-27T18:00:01Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech","hep-th"],"title_canon_sha256":"55a5c90408635d04ab91194d3e621742edb0b33ff569a48c39a57006feaea9a5","abstract_canon_sha256":"3c0096352e906302e6f1fdbcea04f91cf27654be2338e6b1362e348924737109"},"schema_version":"1.0"},"canonical_sha256":"aca75894751dca3383a72c3306d6d7579aea77ad88e068848165fdf863f0f185","source":{"kind":"arxiv","id":"2408.15325","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.15325","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"arxiv_version","alias_value":"2408.15325v2","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.15325","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"pith_short_12","alias_value":"VSTVRFDVDXFD","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"pith_short_16","alias_value":"VSTVRFDVDXFDHA5H","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"pith_short_8","alias_value":"VSTVRFDV","created_at":"2026-07-05T11:18:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:VSTVRFDVDXFDHA5HFQZQNVWXK6","target":"record","payload":{"canonical_record":{"source":{"id":"2408.15325","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-08-27T18:00:01Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech","hep-th"],"title_canon_sha256":"55a5c90408635d04ab91194d3e621742edb0b33ff569a48c39a57006feaea9a5","abstract_canon_sha256":"3c0096352e906302e6f1fdbcea04f91cf27654be2338e6b1362e348924737109"},"schema_version":"1.0"},"canonical_sha256":"aca75894751dca3383a72c3306d6d7579aea77ad88e068848165fdf863f0f185","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:18:39.488039Z","signature_b64":"awjO+jAydufZU7Lr1fNNfx+LTt5PwpPcZti5DpYRSVJu7BqooihiYCVIgsN52TDsOqli69RT7lAy+2+ynCB/BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aca75894751dca3383a72c3306d6d7579aea77ad88e068848165fdf863f0f185","last_reissued_at":"2026-07-05T11:18:39.487571Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:18:39.487571Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2408.15325","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":"2026-07-05T11:18:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5Ax5B+pZL3X2cUIHbaxGwjsjfF0+aaY8OETkG2wQa4eEjOpVcagxLgyAYwuS/BMf7tpqbQ1pjGP+h5QZUILQCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T20:03:26.196154Z"},"content_sha256":"3170b8f4ae8b00ac030a9e82e6667d96296ab29a9fb70e86f61262fb8aa39e51","schema_version":"1.0","event_id":"sha256:3170b8f4ae8b00ac030a9e82e6667d96296ab29a9fb70e86f61262fb8aa39e51"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:VSTVRFDVDXFDHA5HFQZQNVWXK6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Deep thermalization under charge-conserving quantum dynamics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech","hep-th"],"primary_cat":"quant-ph","authors_text":"Harshank Shrotriya, Matteo Ippoliti, Rui-An Chang, Wen Wei Ho","submitted_at":"2024-08-27T18:00:01Z","abstract_excerpt":"\"Deep thermalization\" describes the emergence of universal wavefunction distributions in quantum many-body dynamics, appearing on a local subsystem upon measurement of its environment. In this work, we study in detail the effect of continuous internal symmetries and associated conservation laws on deep thermalization. Concretely, we consider quantum spin systems with a $U(1)$ symmetry associated with the conservation of magnetization (or `charge'), and analyze how the choice of initial states (specifically, their degree of charge fluctuations) and the choice of measurement basis (specifically,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.15325","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2408.15325/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:18:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yyN21ipcKix219fAACvJTaC/kQj129uWFn56VH8Xd2x18/vkRQ21hw/q6I28oSSBmS4+VU7dc6NuMfxp6qBJDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T20:03:26.196663Z"},"content_sha256":"8ec25bdde457af919bf1838d871d3a903e111a95483d39321e83c8527e1b52d8","schema_version":"1.0","event_id":"sha256:8ec25bdde457af919bf1838d871d3a903e111a95483d39321e83c8527e1b52d8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VSTVRFDVDXFDHA5HFQZQNVWXK6/bundle.json","state_url":"https://pith.science/pith/VSTVRFDVDXFDHA5HFQZQNVWXK6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VSTVRFDVDXFDHA5HFQZQNVWXK6/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":"2026-08-10T20:03:26Z","links":{"resolver":"https://pith.science/pith/VSTVRFDVDXFDHA5HFQZQNVWXK6","bundle":"https://pith.science/pith/VSTVRFDVDXFDHA5HFQZQNVWXK6/bundle.json","state":"https://pith.science/pith/VSTVRFDVDXFDHA5HFQZQNVWXK6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VSTVRFDVDXFDHA5HFQZQNVWXK6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:VSTVRFDVDXFDHA5HFQZQNVWXK6","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":"3c0096352e906302e6f1fdbcea04f91cf27654be2338e6b1362e348924737109","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-08-27T18:00:01Z","title_canon_sha256":"55a5c90408635d04ab91194d3e621742edb0b33ff569a48c39a57006feaea9a5"},"schema_version":"1.0","source":{"id":"2408.15325","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.15325","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"arxiv_version","alias_value":"2408.15325v2","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.15325","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"pith_short_12","alias_value":"VSTVRFDVDXFD","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"pith_short_16","alias_value":"VSTVRFDVDXFDHA5H","created_at":"2026-07-05T11:18:39Z"},{"alias_kind":"pith_short_8","alias_value":"VSTVRFDV","created_at":"2026-07-05T11:18:39Z"}],"graph_snapshots":[{"event_id":"sha256:8ec25bdde457af919bf1838d871d3a903e111a95483d39321e83c8527e1b52d8","target":"graph","created_at":"2026-07-05T11:18:39Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2408.15325/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"\"Deep thermalization\" describes the emergence of universal wavefunction distributions in quantum many-body dynamics, appearing on a local subsystem upon measurement of its environment. In this work, we study in detail the effect of continuous internal symmetries and associated conservation laws on deep thermalization. Concretely, we consider quantum spin systems with a $U(1)$ symmetry associated with the conservation of magnetization (or `charge'), and analyze how the choice of initial states (specifically, their degree of charge fluctuations) and the choice of measurement basis (specifically,","authors_text":"Harshank Shrotriya, Matteo Ippoliti, Rui-An Chang, Wen Wei Ho","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech","hep-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-08-27T18:00:01Z","title":"Deep thermalization under charge-conserving quantum dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.15325","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":"sha256:3170b8f4ae8b00ac030a9e82e6667d96296ab29a9fb70e86f61262fb8aa39e51","target":"record","created_at":"2026-07-05T11:18:39Z","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":"3c0096352e906302e6f1fdbcea04f91cf27654be2338e6b1362e348924737109","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-08-27T18:00:01Z","title_canon_sha256":"55a5c90408635d04ab91194d3e621742edb0b33ff569a48c39a57006feaea9a5"},"schema_version":"1.0","source":{"id":"2408.15325","kind":"arxiv","version":2}},"canonical_sha256":"aca75894751dca3383a72c3306d6d7579aea77ad88e068848165fdf863f0f185","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aca75894751dca3383a72c3306d6d7579aea77ad88e068848165fdf863f0f185","first_computed_at":"2026-07-05T11:18:39.487571Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:18:39.487571Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"awjO+jAydufZU7Lr1fNNfx+LTt5PwpPcZti5DpYRSVJu7BqooihiYCVIgsN52TDsOqli69RT7lAy+2+ynCB/BA==","signature_status":"signed_v1","signed_at":"2026-07-05T11:18:39.488039Z","signed_message":"canonical_sha256_bytes"},"source_id":"2408.15325","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3170b8f4ae8b00ac030a9e82e6667d96296ab29a9fb70e86f61262fb8aa39e51","sha256:8ec25bdde457af919bf1838d871d3a903e111a95483d39321e83c8527e1b52d8"],"state_sha256":"c3f86e315ea62476c892feee97d94836d21b17355874d79bce97f7eea9bcb694"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v8ykHyt5sFwNswO3f2QK+teOQHLvG+AKbrge0iX79kFYA3lwe0o8J0QsXDUH+0BqSyDh9gQDpEoYgqYnvv5dDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-10T20:03:26.201270Z","bundle_sha256":"aae299a6a5482957e13032b8528203b86286218834a58dfdfd65705d2dda4f26"}}