{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:XKWRZYIIJSAFGOMWSTJUEIMXL5","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":"a00692ae7afacec0dea1ed133a636abaaa5b91886c37bc34113967669fdb73d2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-11-18T04:14:01Z","title_canon_sha256":"e36d2e7cd24148d0dd628066a0785e003a848657984e73127788e24953a7a91b"},"schema_version":"1.0","source":{"id":"1711.06810","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.06810","created_at":"2026-05-18T00:30:15Z"},{"alias_kind":"arxiv_version","alias_value":"1711.06810v1","created_at":"2026-05-18T00:30:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.06810","created_at":"2026-05-18T00:30:15Z"},{"alias_kind":"pith_short_12","alias_value":"XKWRZYIIJSAF","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"XKWRZYIIJSAFGOMW","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"XKWRZYII","created_at":"2026-05-18T12:31:56Z"}],"graph_snapshots":[{"event_id":"sha256:4c4681409ddad9b0b916c0f09c5a86f902cb2cade525a0bbf8c15da009517094","target":"graph","created_at":"2026-05-18T00:30:15Z","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"},"paper":{"abstract_excerpt":"Computational imaging through scatter generally is accomplished by first characterizing the scattering medium so that its forward operator is obtained; and then imposing additional priors in the form of regularizers on the reconstruction functional so as to improve the condition of the originally ill-posed inverse problem. In the functional, the forward operator and regularizer must be entered explicitly or parametrically (e.g. scattering matrices and dictionaries, respectively.) However, the process of determining these representations is often incomplete, prone to errors, or infeasible. Rece","authors_text":"Ayan Sinha, George Barbastathis, Justin Lee, Mo Deng, Shuai Li","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-11-18T04:14:01Z","title":"Imaging through glass diffusers using densely connected convolutional networks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.06810","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":"sha256:301868a809a03a6746835c6633c78c563827dff516d7726eb980315bd9a99b00","target":"record","created_at":"2026-05-18T00:30:15Z","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":"a00692ae7afacec0dea1ed133a636abaaa5b91886c37bc34113967669fdb73d2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-11-18T04:14:01Z","title_canon_sha256":"e36d2e7cd24148d0dd628066a0785e003a848657984e73127788e24953a7a91b"},"schema_version":"1.0","source":{"id":"1711.06810","kind":"arxiv","version":1}},"canonical_sha256":"baad1ce1084c8053399694d34221975f6e62db01e1073ce985e8f13bf45e3ea4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"baad1ce1084c8053399694d34221975f6e62db01e1073ce985e8f13bf45e3ea4","first_computed_at":"2026-05-18T00:30:15.546837Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:30:15.546837Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"haP3xkmZACuRae7QGyKM1NyZbMxw4zM4vXhAQHYaODm+j7y4q71laXchvjdQJiMAI7mP2HVEi+NxPW6K1ESlDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:30:15.547568Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.06810","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:301868a809a03a6746835c6633c78c563827dff516d7726eb980315bd9a99b00","sha256:4c4681409ddad9b0b916c0f09c5a86f902cb2cade525a0bbf8c15da009517094"],"state_sha256":"0ce64265aacc5296c3313bf59c11728c8706c0c93a46dddeaa1b72ff824c4e81"}