{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:PSDZZAAAOXAVQ2BTDZFQHW4IMP","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":"4610cbc3a0f60c764c3d4b8ce63f67a2ee8642dcc3e98ba7425d9ba59e5ea6da","cross_cats_sorted":["physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-17T10:12:51Z","title_canon_sha256":"9365c21f2d4ccca10dbff0e9a7490e2f4da5802858e52ea4af568da660be2b6e"},"schema_version":"1.0","source":{"id":"2606.18896","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.18896","created_at":"2026-06-19T16:11:51Z"},{"alias_kind":"arxiv_version","alias_value":"2606.18896v1","created_at":"2026-06-19T16:11:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.18896","created_at":"2026-06-19T16:11:51Z"},{"alias_kind":"pith_short_12","alias_value":"PSDZZAAAOXAV","created_at":"2026-06-19T16:11:51Z"},{"alias_kind":"pith_short_16","alias_value":"PSDZZAAAOXAVQ2BT","created_at":"2026-06-19T16:11:51Z"},{"alias_kind":"pith_short_8","alias_value":"PSDZZAAA","created_at":"2026-06-19T16:11:51Z"}],"graph_snapshots":[{"event_id":"sha256:adc120186254fd9e9ab842903ac742bc1efa23e2d73628d11a83b298eeb20634","target":"graph","created_at":"2026-06-19T16:11:51Z","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/2606.18896/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate equilibrium and non-equilibrium thermodynamics of one-dimensional photonic diamond lattices with Kerr nonlinearity. The equilibrium phase diagram is obtained as a function of the synthetic magnetic flux acting on each plaquette. In the linear regime, the magnetic flux can induce Aharonov-Bohm caging, flattening all Bloch bands and suppressing particle and energy currents. In this caging regime, non-vanishing currents are enabled by nonlinearity. By imposing stationary temperature- and chemical potential- imbalances at the system boundaries, we show that at weak nonlinearity fine","authors_text":"Carlo Danieli, Stefano Iubini","cross_cats":["physics.optics"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-17T10:12:51Z","title":"Thermodynamics of photonic nonlinear Aharonov-Bohm cages"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.18896","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:a03d4c3721d47efb30475bb4241091026cd2c9833bdcebe80b004ef840b56681","target":"record","created_at":"2026-06-19T16:11:51Z","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":"4610cbc3a0f60c764c3d4b8ce63f67a2ee8642dcc3e98ba7425d9ba59e5ea6da","cross_cats_sorted":["physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-17T10:12:51Z","title_canon_sha256":"9365c21f2d4ccca10dbff0e9a7490e2f4da5802858e52ea4af568da660be2b6e"},"schema_version":"1.0","source":{"id":"2606.18896","kind":"arxiv","version":1}},"canonical_sha256":"7c879c800075c15868331e4b03db8863c5f9d17202654a06e4e66a45411b9fa1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7c879c800075c15868331e4b03db8863c5f9d17202654a06e4e66a45411b9fa1","first_computed_at":"2026-06-19T16:11:51.263627Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-19T16:11:51.263627Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"iZULm0UE4p3AjF+Nbc0mu0f46dFZtsEfhzmiohPw5x8lCRhOeyvqFkENiQ7oD3xYhorJkd12uG0YgfLXD7rSCA==","signature_status":"signed_v1","signed_at":"2026-06-19T16:11:51.264003Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.18896","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a03d4c3721d47efb30475bb4241091026cd2c9833bdcebe80b004ef840b56681","sha256:adc120186254fd9e9ab842903ac742bc1efa23e2d73628d11a83b298eeb20634"],"state_sha256":"6d4cb1b53bf8e053989459024c0f788c2152742d19b9ea398a5d870cdf142d28"}