{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:YITZP3ZLAJFH6XN3ZNXDTZQJWQ","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":"a160d5f4838e002bf5a959e509bc99bf28bf89c79468bdbcdba10b98bd141f2a","cross_cats_sorted":["cs.IT","math-ph","math.IT","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2020-11-16T15:16:13Z","title_canon_sha256":"2fd30365a3b0b83e71ea0b86712a58ad740c6d1a892e5086beb6d42d515ad96e"},"schema_version":"1.0","source":{"id":"2011.08020","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2011.08020","created_at":"2026-07-05T09:10:39Z"},{"alias_kind":"arxiv_version","alias_value":"2011.08020v3","created_at":"2026-07-05T09:10:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2011.08020","created_at":"2026-07-05T09:10:39Z"},{"alias_kind":"pith_short_12","alias_value":"YITZP3ZLAJFH","created_at":"2026-07-05T09:10:39Z"},{"alias_kind":"pith_short_16","alias_value":"YITZP3ZLAJFH6XN3","created_at":"2026-07-05T09:10:39Z"},{"alias_kind":"pith_short_8","alias_value":"YITZP3ZL","created_at":"2026-07-05T09:10:39Z"}],"graph_snapshots":[{"event_id":"sha256:1936cc729d6207749a8a2ddf167f5f7d98a900ddb49e0091a79910033dcd6f22","target":"graph","created_at":"2026-07-05T09:10:39Z","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/2011.08020/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We consider a theory of quantum thermodynamics with multiple conserved quantities (or charges). To this end, we generalize the seminal results of Sparaciari et al. [PRA 96:052112, 2017] to the case of multiple, in general non-commuting charges, for which we formulate a resource theory of thermodynamics of asymptotically many non-interacting systems. To every state we associate the vector of its expected charge values and its entropy, forming the phase diagram of the system. Our fundamental result is the Asymptotic Equivalence Theorem (AET), which allows us to identify the equivalence classes o","authors_text":"Andreas Winter, Arnau Riera, Maciej Lewenstein, Manabendra Nath Bera, Zahra Baghali Khanian","cross_cats":["cs.IT","math-ph","math.IT","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2020-11-16T15:16:13Z","title":"Resource theory of heat and work with non-commuting charges"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2011.08020","kind":"arxiv","version":3},"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":"sha256:370ea2c077ec17fd9d814d2085728ca0824b49f5d322616a2a5a309e4bfb0633","target":"record","created_at":"2026-07-05T09:10:39Z","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":"a160d5f4838e002bf5a959e509bc99bf28bf89c79468bdbcdba10b98bd141f2a","cross_cats_sorted":["cs.IT","math-ph","math.IT","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2020-11-16T15:16:13Z","title_canon_sha256":"2fd30365a3b0b83e71ea0b86712a58ad740c6d1a892e5086beb6d42d515ad96e"},"schema_version":"1.0","source":{"id":"2011.08020","kind":"arxiv","version":3}},"canonical_sha256":"c22797ef2b024a7f5dbbcb6e39e609b4114760197d7e63cbe5e6b80003e3cae6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c22797ef2b024a7f5dbbcb6e39e609b4114760197d7e63cbe5e6b80003e3cae6","first_computed_at":"2026-07-05T09:10:39.321244Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:10:39.321244Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EToP+ovwsNqIFr82se6SXMsxR4qpBrBhtwderzwLrWb0YbuNWTHsKpmUvzWr7akXpcIcY4BEiGbx+natmf5nAg==","signature_status":"signed_v1","signed_at":"2026-07-05T09:10:39.321708Z","signed_message":"canonical_sha256_bytes"},"source_id":"2011.08020","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:370ea2c077ec17fd9d814d2085728ca0824b49f5d322616a2a5a309e4bfb0633","sha256:1936cc729d6207749a8a2ddf167f5f7d98a900ddb49e0091a79910033dcd6f22"],"state_sha256":"73a4e51a4dab4d1e513de12e8357ed097596a031fb617a35f428bbcdb666a05e"}