{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:DBS2FHQUI7BF7IBYURF2WLRBIH","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":"6794b2fea7757301577eda27bb952b662f12256dee53ef6acb64a235534c420a","cross_cats_sorted":["physics.app-ph","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2024-04-13T09:45:46Z","title_canon_sha256":"4b9f2bfb6c3debbb6d57d533150bcb7410109d9f1578a858fd2d2e2407cb9850"},"schema_version":"1.0","source":{"id":"2404.08946","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.08946","created_at":"2026-07-05T08:07:42Z"},{"alias_kind":"arxiv_version","alias_value":"2404.08946v1","created_at":"2026-07-05T08:07:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.08946","created_at":"2026-07-05T08:07:42Z"},{"alias_kind":"pith_short_12","alias_value":"DBS2FHQUI7BF","created_at":"2026-07-05T08:07:42Z"},{"alias_kind":"pith_short_16","alias_value":"DBS2FHQUI7BF7IBY","created_at":"2026-07-05T08:07:42Z"},{"alias_kind":"pith_short_8","alias_value":"DBS2FHQU","created_at":"2026-07-05T08:07:42Z"}],"graph_snapshots":[{"event_id":"sha256:c2b3b0255ebfca652f6223630354061151565ad0e5ee5f413c5332b08f7e4b7d","target":"graph","created_at":"2026-07-05T08:07:42Z","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/2404.08946/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Confocal laser scanning microscopy (CLSM) stands out as one of the most widely used microscopy techniques, thanks to its three-dimensional imaging capability and its sub-diffraction spatial resolution, achieved through the closure of a pinhole in front of a single-element detector. However, the pinhole also rejects useful photons and beating the diffraction limit comes at the price of irremediably compromising the signal-to-noise ratio (SNR) of the data. Image scanning microscopy (ISM) emerged as the natural evolution of CLSM, exploiting a small array detector in place of the pinhole and the s","authors_text":"Alessandro Zunino, Alvaro H. Crevenna, Daniele Ancora, Giuseppe Vicidomini","cross_cats":["physics.app-ph","physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2024-04-13T09:45:46Z","title":"Image Scanning Microscopy Reconstruction by Autocorrelation Inversion"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.08946","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:c046b1c67003c96351c258c1b4a5fbfcfa3fa5238e9e144fad47f2b908a222f7","target":"record","created_at":"2026-07-05T08:07:42Z","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":"6794b2fea7757301577eda27bb952b662f12256dee53ef6acb64a235534c420a","cross_cats_sorted":["physics.app-ph","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2024-04-13T09:45:46Z","title_canon_sha256":"4b9f2bfb6c3debbb6d57d533150bcb7410109d9f1578a858fd2d2e2407cb9850"},"schema_version":"1.0","source":{"id":"2404.08946","kind":"arxiv","version":1}},"canonical_sha256":"1865a29e1447c25fa038a44bab2e2141dc22a2af3fc40ea343a65d34b15250ac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1865a29e1447c25fa038a44bab2e2141dc22a2af3fc40ea343a65d34b15250ac","first_computed_at":"2026-07-05T08:07:42.571251Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:07:42.571251Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bOXjr0neBkmwSj9KwFUG2lM6uii78qWEPOhx6fCPLPy7H4n57GI9xA5QrB8HYdAnQOn2AkPaCxgbAYJ+X8I1CA==","signature_status":"signed_v1","signed_at":"2026-07-05T08:07:42.571643Z","signed_message":"canonical_sha256_bytes"},"source_id":"2404.08946","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c046b1c67003c96351c258c1b4a5fbfcfa3fa5238e9e144fad47f2b908a222f7","sha256:c2b3b0255ebfca652f6223630354061151565ad0e5ee5f413c5332b08f7e4b7d"],"state_sha256":"3db2e505dbe67a56b03712c3fb7511560b4cc6db464b9c6207c7b56ac2c8d7f3"}