{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:ZVOPS3VSQWLWKQRWAUFLUDFN73","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":"f45258f43edcac2616e54b7cc6fcc0e555b0e2e0f00b80eeecb79a2d30819829","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-07-03T07:56:33Z","title_canon_sha256":"50ef69178cfa6c8f472d13759bb49eaca0e9e35a34555995f169f3246d5acb63"},"schema_version":"1.0","source":{"id":"1307.0931","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.0931","created_at":"2026-05-18T03:19:14Z"},{"alias_kind":"arxiv_version","alias_value":"1307.0931v1","created_at":"2026-05-18T03:19:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.0931","created_at":"2026-05-18T03:19:14Z"},{"alias_kind":"pith_short_12","alias_value":"ZVOPS3VSQWLW","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"ZVOPS3VSQWLWKQRW","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"ZVOPS3VS","created_at":"2026-05-18T12:28:09Z"}],"graph_snapshots":[{"event_id":"sha256:d6b2e959c0a3beb5d3121f9a69c002ae5b5941e0474fd218b8bf72b26e18cbb6","target":"graph","created_at":"2026-05-18T03:19:14Z","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":"We demonstrate applications of a novel setup which is used for measuring relative phase difference between S and P polarization at oblique incidence point in optically denser medium by analyzing the relative frequency shift of adjacent axial modes of S and P resonances of a monolithic folded Fabry-Perot cavity (MFC). The relative frequency shift of adjacent axial modes of S and P resonances of MFC is around 1.030 GHz for the confocal MFC cavity and 0.3869 GHz for the parallel MFC cavity respectively. The relative phase difference at reflection point A in optically denser medium is inferred to ","authors_text":"Yu Peng","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-07-03T07:56:33Z","title":"A novel scheme for measuring the relative phase difference between S and P polarization in optically denser medium"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.0931","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:c1c4aad495b43ca4fb439d68dad17fec47931a5e4bec06e405c1aaf75676ded1","target":"record","created_at":"2026-05-18T03:19:14Z","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":"f45258f43edcac2616e54b7cc6fcc0e555b0e2e0f00b80eeecb79a2d30819829","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2013-07-03T07:56:33Z","title_canon_sha256":"50ef69178cfa6c8f472d13759bb49eaca0e9e35a34555995f169f3246d5acb63"},"schema_version":"1.0","source":{"id":"1307.0931","kind":"arxiv","version":1}},"canonical_sha256":"cd5cf96eb28597654236050aba0cadfed3baaffb3581406df7e6bade729ddfa0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cd5cf96eb28597654236050aba0cadfed3baaffb3581406df7e6bade729ddfa0","first_computed_at":"2026-05-18T03:19:14.633969Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:19:14.633969Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pwf8mX4edF9eFN7dUSCjzhBHAjEIUq/SU19kVPooLFmj8Pjhj4VhMMwmJMwDfJXgAHQ+VhSIPfjoXnlf+BQ1Bw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:19:14.634512Z","signed_message":"canonical_sha256_bytes"},"source_id":"1307.0931","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c1c4aad495b43ca4fb439d68dad17fec47931a5e4bec06e405c1aaf75676ded1","sha256:d6b2e959c0a3beb5d3121f9a69c002ae5b5941e0474fd218b8bf72b26e18cbb6"],"state_sha256":"54f001965568a96605c560f5e308074c64a3fd57b8ae6a8fc8cad20e6ed1bb09"}