{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:JXDLSTXIPDVACUTHMTJ363DKJW","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":"06e1bf5100e1604cdf3d8e40c6276b3aec49ebf5918d7edab1b1790eddb255fc","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-08T14:18:16Z","title_canon_sha256":"b3a66850b3932dd70096b0a1c5805c29a737381052f5448f8befdddcc7ab58c8"},"schema_version":"1.0","source":{"id":"2403.05341","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2403.05341","created_at":"2026-07-05T07:53:54Z"},{"alias_kind":"arxiv_version","alias_value":"2403.05341v1","created_at":"2026-07-05T07:53:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.05341","created_at":"2026-07-05T07:53:54Z"},{"alias_kind":"pith_short_12","alias_value":"JXDLSTXIPDVA","created_at":"2026-07-05T07:53:54Z"},{"alias_kind":"pith_short_16","alias_value":"JXDLSTXIPDVACUTH","created_at":"2026-07-05T07:53:54Z"},{"alias_kind":"pith_short_8","alias_value":"JXDLSTXI","created_at":"2026-07-05T07:53:54Z"}],"graph_snapshots":[{"event_id":"sha256:d4b5d84fb623d63fe2cb3ecc9ab0a3cd5b22755d4c3cf5e6ce6eb3dd550b7b40","target":"graph","created_at":"2026-07-05T07:53:54Z","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/2403.05341/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"As a highly sensitive vibrational imaging method, stimulated Raman scattering (SRS) microscopy is finding various applications, while its theoretical treatment seems still under development. Here we present a theoretical estimation of spontaneous Raman signal and SRS signal from Raman scattering cross section, irrespective of the numerical aperture of the objective lens. We confirm a reasonable agreement between our theory with a recently proposed treatment based on the stimulated Raman scattering cross section. Furthermore, we point out that the acceleration factor of SRS can be interpreted a","authors_text":"Yasuyuki Ozeki","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-08T14:18:16Z","title":"Theoretical estimation of stimulated and spontaneous Raman signals in Raman microscopy"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.05341","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:fb0936704c31e304e6318133feb2e8f353a41d76bca509688c0c28ab96ebfef1","target":"record","created_at":"2026-07-05T07:53:54Z","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":"06e1bf5100e1604cdf3d8e40c6276b3aec49ebf5918d7edab1b1790eddb255fc","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-08T14:18:16Z","title_canon_sha256":"b3a66850b3932dd70096b0a1c5805c29a737381052f5448f8befdddcc7ab58c8"},"schema_version":"1.0","source":{"id":"2403.05341","kind":"arxiv","version":1}},"canonical_sha256":"4dc6b94ee878ea01526764d3bf6c6a4d96a536c374384f9fec51ce50616e9a14","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4dc6b94ee878ea01526764d3bf6c6a4d96a536c374384f9fec51ce50616e9a14","first_computed_at":"2026-07-05T07:53:54.067001Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:53:54.067001Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qj+q9cBD2zmwwJ6lXR6IDi3xaFoBlu0kxZKPxQ9PPsAadnzgnabI235M+BJzzZff9a2bIKGaB0DbclNi8zWvCw==","signature_status":"signed_v1","signed_at":"2026-07-05T07:53:54.067465Z","signed_message":"canonical_sha256_bytes"},"source_id":"2403.05341","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fb0936704c31e304e6318133feb2e8f353a41d76bca509688c0c28ab96ebfef1","sha256:d4b5d84fb623d63fe2cb3ecc9ab0a3cd5b22755d4c3cf5e6ce6eb3dd550b7b40"],"state_sha256":"d41df104fc7b551c22ff41a32089fd049b92b67c0b41a70b7ffee71fbc80dbe7"}