{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:TGEG5SHZQTGRWINUY525G66CFG","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":"295496b39a7e46f886a2e0a2492a60294bb986366ad90575c31731a1e5626b03","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.quant-gas","cond-mat.stat-mech","cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-09-16T14:04:38Z","title_canon_sha256":"7cdd2189e0e043b7fd0bedb01a49f9dc6862cba9dadd521ef5e491c33b5fa5e2"},"schema_version":"1.0","source":{"id":"2409.10300","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.10300","created_at":"2026-07-05T11:56:00Z"},{"alias_kind":"arxiv_version","alias_value":"2409.10300v4","created_at":"2026-07-05T11:56:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.10300","created_at":"2026-07-05T11:56:00Z"},{"alias_kind":"pith_short_12","alias_value":"TGEG5SHZQTGR","created_at":"2026-07-05T11:56:00Z"},{"alias_kind":"pith_short_16","alias_value":"TGEG5SHZQTGRWINU","created_at":"2026-07-05T11:56:00Z"},{"alias_kind":"pith_short_8","alias_value":"TGEG5SHZ","created_at":"2026-07-05T11:56:00Z"}],"graph_snapshots":[{"event_id":"sha256:145aa9d8f669adda50d1efa44cd97f03ebcbc17fa099c1a984e3662bf9eea70d","target":"graph","created_at":"2026-07-05T11:56:00Z","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/2409.10300/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"These Lecture Notes discuss the recent theoretical advances in the understanding of open quantum many-body physics in platforms where both dissipative and coherent processes can be tuned and controlled to a high degree. We start by reviewing the theoretical frameworks and methods used to describe and tackle open quantum many-body systems. We then discuss the use of dissipative processes to engineer many-body stationary states with desired properties and the emergence of dissipative phase transitions arising out of the competition between coherent evolution and dissipation. We review the dynami","authors_text":"Jonathan Keeling, Leonardo Mazza, Marco Schir\\`o, Rosario Fazio","cross_cats":["cond-mat.mes-hall","cond-mat.quant-gas","cond-mat.stat-mech","cond-mat.str-el"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-09-16T14:04:38Z","title":"Many-Body Open Quantum Systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.10300","kind":"arxiv","version":4},"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":"sha256:48f20e2c87cbacc271dab344c6052f7e52f3e83a187e85dc7f3972b625510aa3","target":"record","created_at":"2026-07-05T11:56:00Z","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":"295496b39a7e46f886a2e0a2492a60294bb986366ad90575c31731a1e5626b03","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.quant-gas","cond-mat.stat-mech","cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-09-16T14:04:38Z","title_canon_sha256":"7cdd2189e0e043b7fd0bedb01a49f9dc6862cba9dadd521ef5e491c33b5fa5e2"},"schema_version":"1.0","source":{"id":"2409.10300","kind":"arxiv","version":4}},"canonical_sha256":"99886ec8f984cd1b21b4c775d37bc229a8edb5719f17d93ddf951d4a949d5c47","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"99886ec8f984cd1b21b4c775d37bc229a8edb5719f17d93ddf951d4a949d5c47","first_computed_at":"2026-07-05T11:56:00.611608Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:56:00.611608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"u1ELNMbp2JHxCSju2kMqivjSF8w5lOyR8a5Zdk5OBVTC1OsxvUAAZe0r3mArYr0LZvRs8UK0aq+RIqC8AR++Aw==","signature_status":"signed_v1","signed_at":"2026-07-05T11:56:00.612054Z","signed_message":"canonical_sha256_bytes"},"source_id":"2409.10300","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:48f20e2c87cbacc271dab344c6052f7e52f3e83a187e85dc7f3972b625510aa3","sha256:145aa9d8f669adda50d1efa44cd97f03ebcbc17fa099c1a984e3662bf9eea70d"],"state_sha256":"03c7df8d4b6ad6917f00e5f3060292acfaa0d804bc46aa16306c4ae450384ad2"}