{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:CIMKGADCAGXHWOSMZ7VEWCSG4X","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":"eee9d34c159d937425053547b42d81260cc722a95015ffa3427e017661ea5e5f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-07-07T04:40:10Z","title_canon_sha256":"ec4ca06968d3b2ccea0eb69b7d681663bd37128fccb616d3bd94f3cf13fefd74"},"schema_version":"1.0","source":{"id":"2607.05824","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.05824","created_at":"2026-07-08T01:18:47Z"},{"alias_kind":"arxiv_version","alias_value":"2607.05824v1","created_at":"2026-07-08T01:18:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.05824","created_at":"2026-07-08T01:18:47Z"},{"alias_kind":"pith_short_12","alias_value":"CIMKGADCAGXH","created_at":"2026-07-08T01:18:47Z"},{"alias_kind":"pith_short_16","alias_value":"CIMKGADCAGXHWOSM","created_at":"2026-07-08T01:18:47Z"},{"alias_kind":"pith_short_8","alias_value":"CIMKGADC","created_at":"2026-07-08T01:18:47Z"}],"graph_snapshots":[{"event_id":"sha256:205e8a2f95347858dbb3b98dd52c9fd993351874d7f080a6ff5047125fc4ba79","target":"graph","created_at":"2026-07-08T01:18:47Z","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/2607.05824/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"High-throughput holotomography often relies on long-working-distance, multiwell-compatible optics that reduce illumination numerical aperture (NA) and limit access to high spatial frequencies. Here we present ResShift-ODE, a deterministic diffusion-prior framework that transfers low-NA refractive-index (RI) tomograms to high-NA-equivalent volumes without modifying the acquisition hardware. We formulate low-NA-to-high-NA transfer as a diffusion-prior inverse problem under an explicit NA-limited Fourier-domain forward operator, distinct from suppressing artifacts within an already measured passb","authors_text":"Dong-min Ryu, Hansol Yoon, Hyun-seok Min, Jeong-hyun Roh, Woon-soo Lee, YongKeun Park","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-07-07T04:40:10Z","title":"Numerical-aperture transfer in holotomography with a deterministic diffusion prior"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.05824","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":"sha256:0987bca9bc90ca3a8c679d4c96109ca039395215abaa5602a57ffb7a56f9a98e","target":"record","created_at":"2026-07-08T01:18:47Z","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":"eee9d34c159d937425053547b42d81260cc722a95015ffa3427e017661ea5e5f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-07-07T04:40:10Z","title_canon_sha256":"ec4ca06968d3b2ccea0eb69b7d681663bd37128fccb616d3bd94f3cf13fefd74"},"schema_version":"1.0","source":{"id":"2607.05824","kind":"arxiv","version":1}},"canonical_sha256":"1218a3006201ae7b3a4ccfea4b0a46e5d73b37d1e40769c2e8731c2e8447fc97","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1218a3006201ae7b3a4ccfea4b0a46e5d73b37d1e40769c2e8731c2e8447fc97","first_computed_at":"2026-07-08T01:18:47.106665Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-08T01:18:47.106665Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8hl2OXe1q4T3aam+u91L3K/MuK2TinLKNsFcQoIP9NhE3x1QxHd86FUTjPSKZmhNt7EhKf6CEJoa2kNBoU44DQ==","signature_status":"signed_v1","signed_at":"2026-07-08T01:18:47.107211Z","signed_message":"canonical_sha256_bytes"},"source_id":"2607.05824","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0987bca9bc90ca3a8c679d4c96109ca039395215abaa5602a57ffb7a56f9a98e","sha256:205e8a2f95347858dbb3b98dd52c9fd993351874d7f080a6ff5047125fc4ba79"],"state_sha256":"5b909e25a6fec9ecafda877c61ac2797a1451fe161f8bf6aac8537739e66e9e7"}