{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:D64OQIDFS5OBVDYLKBCACGAYS5","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":"47ee777857c9322b02409a14235f42aa84721524ff97b4843b4fe8501f70073a","cross_cats_sorted":["physics.bio-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-02T06:04:50Z","title_canon_sha256":"3ac9b65f5ec8b939f6ee77c0a8b93cf94fe2a92e1b08335e418317604de686b9"},"schema_version":"1.0","source":{"id":"2606.03205","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.03205","created_at":"2026-06-03T01:05:34Z"},{"alias_kind":"arxiv_version","alias_value":"2606.03205v1","created_at":"2026-06-03T01:05:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.03205","created_at":"2026-06-03T01:05:34Z"},{"alias_kind":"pith_short_12","alias_value":"D64OQIDFS5OB","created_at":"2026-06-03T01:05:34Z"},{"alias_kind":"pith_short_16","alias_value":"D64OQIDFS5OBVDYL","created_at":"2026-06-03T01:05:34Z"},{"alias_kind":"pith_short_8","alias_value":"D64OQIDF","created_at":"2026-06-03T01:05:34Z"}],"graph_snapshots":[{"event_id":"sha256:b2937b291622446d34210125c0d40e316d0658f19387c3a26c88033d27912e61","target":"graph","created_at":"2026-06-03T01:05:34Z","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/2606.03205/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Optimizing energy conversion in active matter remains a central challenge in nonequilibrium physics. Here, we develop a unified thermodynamic framework that characterizes the finite-time performance of interacting active machines. We show that cyclic work admits a geometric decomposition into an antisymmetric thermodynamic curvature, governing work extraction, and a symmetric metric, controlling dissipation. Minimal-dissipation protocols follow geodesics in parameter space, while optimal work extraction deviates from them due to a curvature-induced, Lorentz-like effect. This geometric structur","authors_text":"Geng Li, Z. C. Tu","cross_cats":["physics.bio-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-02T06:04:50Z","title":"Geometric Bounds on the Finite-Time Performance of Active Machines"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.03205","kind":"arxiv","version":1},"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":"sha256:7da01e150dfad0a24d2b54fdc3963f860a6a40819964048e951105b4b23feabc","target":"record","created_at":"2026-06-03T01:05:34Z","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":"47ee777857c9322b02409a14235f42aa84721524ff97b4843b4fe8501f70073a","cross_cats_sorted":["physics.bio-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-02T06:04:50Z","title_canon_sha256":"3ac9b65f5ec8b939f6ee77c0a8b93cf94fe2a92e1b08335e418317604de686b9"},"schema_version":"1.0","source":{"id":"2606.03205","kind":"arxiv","version":1}},"canonical_sha256":"1fb8e82065975c1a8f0b50440118189746d8f0292eb83af483f8e820cbd23622","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1fb8e82065975c1a8f0b50440118189746d8f0292eb83af483f8e820cbd23622","first_computed_at":"2026-06-03T01:05:34.853148Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-03T01:05:34.853148Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"m9MU75I0r8xE2fQ6CANawvnWCeoW4/ne15zHobIjhoZW9KGGXMygN1yd2SjBe05xAeRRwE1ppaNF3d+VX2ShCQ==","signature_status":"signed_v1","signed_at":"2026-06-03T01:05:34.853533Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.03205","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7da01e150dfad0a24d2b54fdc3963f860a6a40819964048e951105b4b23feabc","sha256:b2937b291622446d34210125c0d40e316d0658f19387c3a26c88033d27912e61"],"state_sha256":"87b3d2da1c268637ed4b7b8f048d7dbba38cb609a711c57a5f3bead8a7629f46"}