{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:BYB4HKOY4NZPKKIWH6LG6M4E3G","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":"6d9a588ffd04bb2dfed18a8bee4ffaca62bfa99d7195e65ab61b27d29a7bd21b","cross_cats_sorted":["cs.LG"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-04-19T03:04:21Z","title_canon_sha256":"233a3b207e5e400bccf66be8a540f490ed3a95783c5cefd694d9021b11182593"},"schema_version":"1.0","source":{"id":"2504.14157","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2504.14157","created_at":"2026-07-05T10:51:11Z"},{"alias_kind":"arxiv_version","alias_value":"2504.14157v1","created_at":"2026-07-05T10:51:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.14157","created_at":"2026-07-05T10:51:11Z"},{"alias_kind":"pith_short_12","alias_value":"BYB4HKOY4NZP","created_at":"2026-07-05T10:51:11Z"},{"alias_kind":"pith_short_16","alias_value":"BYB4HKOY4NZPKKIW","created_at":"2026-07-05T10:51:11Z"},{"alias_kind":"pith_short_8","alias_value":"BYB4HKOY","created_at":"2026-07-05T10:51:11Z"}],"graph_snapshots":[{"event_id":"sha256:15364571be1220e0f8e153c6436c4f43f8a949197132e97d72428024254c201d","target":"graph","created_at":"2026-07-05T10:51:11Z","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/2504.14157/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Sample-induced aberrations and optical imperfections limit the resolution of fluorescence microscopy. Phase diversity is a powerful technique that leverages complementary phase information in sequentially acquired images with deliberately introduced aberrations--the phase diversities--to enable phase and object reconstruction and restore diffraction-limited resolution. These phase diversities are typically introduced into the optical path via a deformable mirror. Existing phase-diversity-based methods are limited to Zernike modes, require large numbers of diversity images, or depend on accurat","authors_text":"Cedric Allier, Courtney Johnson, Diane Adjavon, Hari Shroff, Joren Husic, Larissa Heinrich, Magdalena C. Schneider, Patrick La Rivi\\`ere, Stephan Saalfeld","cross_cats":["cs.LG"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-04-19T03:04:21Z","title":"DeepPD: Joint Phase and Object Estimation from Phase Diversity with Neural Calibration of a Deformable Mirror"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.14157","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":"sha256:6531795a970634a7ef207021001982147c8da8c773ac06629610b6785cce8ad1","target":"record","created_at":"2026-07-05T10:51:11Z","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":"6d9a588ffd04bb2dfed18a8bee4ffaca62bfa99d7195e65ab61b27d29a7bd21b","cross_cats_sorted":["cs.LG"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-04-19T03:04:21Z","title_canon_sha256":"233a3b207e5e400bccf66be8a540f490ed3a95783c5cefd694d9021b11182593"},"schema_version":"1.0","source":{"id":"2504.14157","kind":"arxiv","version":1}},"canonical_sha256":"0e03c3a9d8e372f529163f966f3384d9a7dba154f38cb52e00e1938fb714bf8c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0e03c3a9d8e372f529163f966f3384d9a7dba154f38cb52e00e1938fb714bf8c","first_computed_at":"2026-07-05T10:51:11.981427Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:51:11.981427Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lxNOVI2QeNJ2wm3f8cyAAybMpgGYy7EGTb1leOC/4M9fhoAE4oDk8n0JZmzQsqeYGE90O6KPTeUpbtsQZs8YCg==","signature_status":"signed_v1","signed_at":"2026-07-05T10:51:11.981904Z","signed_message":"canonical_sha256_bytes"},"source_id":"2504.14157","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6531795a970634a7ef207021001982147c8da8c773ac06629610b6785cce8ad1","sha256:15364571be1220e0f8e153c6436c4f43f8a949197132e97d72428024254c201d"],"state_sha256":"6f9a9625235d0d35b7bab24c5db1592d3f3202cbd4c0a44dfff0f883958d9f19"}