{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:VNPMR2SJOJT2NR33QZS7USF5ZS","short_pith_number":"pith:VNPMR2SJ","canonical_record":{"source":{"id":"2505.17754","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-23T11:23:59Z","cross_cats_sorted":["math-ph","math.MP","math.OC"],"title_canon_sha256":"b06263661a099629f457bbf0f99d9f944f3af4383d69fe13d699a655b8503ddb","abstract_canon_sha256":"8b41dce05df31f715e4d08732b2935f64634d2c93cdb60e347ec659dc9673fe9"},"schema_version":"1.0"},"canonical_sha256":"ab5ec8ea497267a6c77b8665fa48bdcca69896c25325a6febd824d37c360a408","source":{"kind":"arxiv","id":"2505.17754","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.17754","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"arxiv_version","alias_value":"2505.17754v1","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.17754","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"pith_short_12","alias_value":"VNPMR2SJOJT2","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"pith_short_16","alias_value":"VNPMR2SJOJT2NR33","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"pith_short_8","alias_value":"VNPMR2SJ","created_at":"2026-07-05T11:08:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:VNPMR2SJOJT2NR33QZS7USF5ZS","target":"record","payload":{"canonical_record":{"source":{"id":"2505.17754","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-23T11:23:59Z","cross_cats_sorted":["math-ph","math.MP","math.OC"],"title_canon_sha256":"b06263661a099629f457bbf0f99d9f944f3af4383d69fe13d699a655b8503ddb","abstract_canon_sha256":"8b41dce05df31f715e4d08732b2935f64634d2c93cdb60e347ec659dc9673fe9"},"schema_version":"1.0"},"canonical_sha256":"ab5ec8ea497267a6c77b8665fa48bdcca69896c25325a6febd824d37c360a408","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:08:31.260804Z","signature_b64":"tJuw3PqD6rFQNojidUJ5gdNkdKF0xfYzZ6Q1n/xGAjXKioZMhU9vRZXSturTQRp4p1N0r069+TdlnV9hZw5PBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ab5ec8ea497267a6c77b8665fa48bdcca69896c25325a6febd824d37c360a408","last_reissued_at":"2026-07-05T11:08:31.260396Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:08:31.260396Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2505.17754","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:08:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8tE1rOLoaNjQXz4NuA7++ApjXkNY1p+5tGOsxaRMRZvSWzCsmw97SLlLerkq5JBflr41XmfusbVkUJ7oaB2fDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T16:42:33.479819Z"},"content_sha256":"21289ab74074ecfaa1aeb60e1c49a52ea1e3e24bb9ae4cf4c2c8011ac5b892d6","schema_version":"1.0","event_id":"sha256:21289ab74074ecfaa1aeb60e1c49a52ea1e3e24bb9ae4cf4c2c8011ac5b892d6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:VNPMR2SJOJT2NR33QZS7USF5ZS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Surface-Encoded Partial Coherence Transformation: Modeling Source Coherence Effects in Wave Optics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["math-ph","math.MP","math.OC"],"primary_cat":"physics.optics","authors_text":"Netzer Moriya","submitted_at":"2025-05-23T11:23:59Z","abstract_excerpt":"We present a new mathematical framework for incorporating partial coherence effects into wave optics simulations through a comprehensive surface-to-detector approach. Unlike traditional ensemble averaging methods, our dual-component framework models partial coherence through: (1) a surface-encoded transformation implemented via a linear integral operator with a spatially-dependent kernel that modifies coherence properties at the reflection interface, followed by (2) a propagation component that evolves these coherence properties to the detection plane. This approach differs fundamentally from "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.17754","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.17754/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:08:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"teW8gNoNFvGHZP6FbhjbrTATYA3/cJDYRIm2Jaw5zu1Fg8Rmz4fKJzhgDBKP/k2J2wY1NR1GF+RlrBZdBnntAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T16:42:33.481679Z"},"content_sha256":"b5d391a5debc47d2ee5135b83abecb738bced713c7d326a404130c8c00187bce","schema_version":"1.0","event_id":"sha256:b5d391a5debc47d2ee5135b83abecb738bced713c7d326a404130c8c00187bce"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VNPMR2SJOJT2NR33QZS7USF5ZS/bundle.json","state_url":"https://pith.science/pith/VNPMR2SJOJT2NR33QZS7USF5ZS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VNPMR2SJOJT2NR33QZS7USF5ZS/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-14T16:42:33Z","links":{"resolver":"https://pith.science/pith/VNPMR2SJOJT2NR33QZS7USF5ZS","bundle":"https://pith.science/pith/VNPMR2SJOJT2NR33QZS7USF5ZS/bundle.json","state":"https://pith.science/pith/VNPMR2SJOJT2NR33QZS7USF5ZS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VNPMR2SJOJT2NR33QZS7USF5ZS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:VNPMR2SJOJT2NR33QZS7USF5ZS","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":"8b41dce05df31f715e4d08732b2935f64634d2c93cdb60e347ec659dc9673fe9","cross_cats_sorted":["math-ph","math.MP","math.OC"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-23T11:23:59Z","title_canon_sha256":"b06263661a099629f457bbf0f99d9f944f3af4383d69fe13d699a655b8503ddb"},"schema_version":"1.0","source":{"id":"2505.17754","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.17754","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"arxiv_version","alias_value":"2505.17754v1","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.17754","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"pith_short_12","alias_value":"VNPMR2SJOJT2","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"pith_short_16","alias_value":"VNPMR2SJOJT2NR33","created_at":"2026-07-05T11:08:31Z"},{"alias_kind":"pith_short_8","alias_value":"VNPMR2SJ","created_at":"2026-07-05T11:08:31Z"}],"graph_snapshots":[{"event_id":"sha256:b5d391a5debc47d2ee5135b83abecb738bced713c7d326a404130c8c00187bce","target":"graph","created_at":"2026-07-05T11:08:31Z","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/2505.17754/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a new mathematical framework for incorporating partial coherence effects into wave optics simulations through a comprehensive surface-to-detector approach. Unlike traditional ensemble averaging methods, our dual-component framework models partial coherence through: (1) a surface-encoded transformation implemented via a linear integral operator with a spatially-dependent kernel that modifies coherence properties at the reflection interface, followed by (2) a propagation component that evolves these coherence properties to the detection plane. This approach differs fundamentally from ","authors_text":"Netzer Moriya","cross_cats":["math-ph","math.MP","math.OC"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-23T11:23:59Z","title":"Surface-Encoded Partial Coherence Transformation: Modeling Source Coherence Effects in Wave Optics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.17754","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":"sha256:21289ab74074ecfaa1aeb60e1c49a52ea1e3e24bb9ae4cf4c2c8011ac5b892d6","target":"record","created_at":"2026-07-05T11:08:31Z","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":"8b41dce05df31f715e4d08732b2935f64634d2c93cdb60e347ec659dc9673fe9","cross_cats_sorted":["math-ph","math.MP","math.OC"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-23T11:23:59Z","title_canon_sha256":"b06263661a099629f457bbf0f99d9f944f3af4383d69fe13d699a655b8503ddb"},"schema_version":"1.0","source":{"id":"2505.17754","kind":"arxiv","version":1}},"canonical_sha256":"ab5ec8ea497267a6c77b8665fa48bdcca69896c25325a6febd824d37c360a408","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ab5ec8ea497267a6c77b8665fa48bdcca69896c25325a6febd824d37c360a408","first_computed_at":"2026-07-05T11:08:31.260396Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:08:31.260396Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tJuw3PqD6rFQNojidUJ5gdNkdKF0xfYzZ6Q1n/xGAjXKioZMhU9vRZXSturTQRp4p1N0r069+TdlnV9hZw5PBg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:08:31.260804Z","signed_message":"canonical_sha256_bytes"},"source_id":"2505.17754","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:21289ab74074ecfaa1aeb60e1c49a52ea1e3e24bb9ae4cf4c2c8011ac5b892d6","sha256:b5d391a5debc47d2ee5135b83abecb738bced713c7d326a404130c8c00187bce"],"state_sha256":"e65c627dbe56a80daac90a2a2cc6938f3f227370792f951e9f5109bd95e5920a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ulmngRvfpK1ioXwBdg+IBUGtoQ2cPw+79N6cAIjcZUZDrzcmz5cUW08Fk/IbFbK7TYuPjKKkVNKJG0Cn0DorAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-14T16:42:33.492691Z","bundle_sha256":"0111855d0e76c8aaeb18deaa7372bc7e0e722c066ece580107e327c5cc192331"}}