{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:QHCU57HS77YINARHHTZEAICGBO","short_pith_number":"pith:QHCU57HS","schema_version":"1.0","canonical_sha256":"81c54efcf2fff08682273cf24020460b84cc7b5e0f1ee8e793c08cf6c808b7c2","source":{"kind":"arxiv","id":"1709.05924","version":2},"attestation_state":"computed","paper":{"title":"Analysis of the design of a passive resonant miniature optical gyroscope based on integrated optics technologies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"2, (2) TAV, 3), (3) LAC), Alexia Ravaille (1, Fabien Bretenaker (3) ((1) TRT, Gilles Feugnet (1), Sylvain Schwartz (1)","submitted_at":"2017-07-14T03:57:15Z","abstract_excerpt":"We present a simple analysis of the design of a passive miniature resonant optical gyroscope. By combining the requirements on the angular random walk and the bias stability, we end up with simple expressions of the minimum diameter of the ring waveguide cavity and the maximum power that should be used to probe it. Using state-of-the-art performances of photonic integrated circuit and whispering gallery mode technologies in terms of propagation losses and mode size, we show that tactical grade gyroscope performances can be achieved with a diameter of a few cm provided the detrimental influence"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1709.05924","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-07-14T03:57:15Z","cross_cats_sorted":[],"title_canon_sha256":"0f5052a2b1451cc0ea27d146a3a9802afaba891b44c83cada635ac57132129c6","abstract_canon_sha256":"a0fc789683c4c9756fdfbbdf2202c2c7127982c4f4d314daddf9a8444c17dbf6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:58:50.138964Z","signature_b64":"Ou4kKIScSBcECJvgBn9ZxHVkYJW3M5mzt1HHkE2Hyrsb+ocXU2VoLzevBlHr1z5ZbQZa5iLMqxl5eqx7HOnLDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"81c54efcf2fff08682273cf24020460b84cc7b5e0f1ee8e793c08cf6c808b7c2","last_reissued_at":"2026-05-17T23:58:50.138168Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:58:50.138168Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis of the design of a passive resonant miniature optical gyroscope based on integrated optics technologies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"2, (2) TAV, 3), (3) LAC), Alexia Ravaille (1, Fabien Bretenaker (3) ((1) TRT, Gilles Feugnet (1), Sylvain Schwartz (1)","submitted_at":"2017-07-14T03:57:15Z","abstract_excerpt":"We present a simple analysis of the design of a passive miniature resonant optical gyroscope. By combining the requirements on the angular random walk and the bias stability, we end up with simple expressions of the minimum diameter of the ring waveguide cavity and the maximum power that should be used to probe it. Using state-of-the-art performances of photonic integrated circuit and whispering gallery mode technologies in terms of propagation losses and mode size, we show that tactical grade gyroscope performances can be achieved with a diameter of a few cm provided the detrimental influence"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.05924","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1709.05924","created_at":"2026-05-17T23:58:50.138271+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.05924v2","created_at":"2026-05-17T23:58:50.138271+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.05924","created_at":"2026-05-17T23:58:50.138271+00:00"},{"alias_kind":"pith_short_12","alias_value":"QHCU57HS77YI","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_16","alias_value":"QHCU57HS77YINARH","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_8","alias_value":"QHCU57HS","created_at":"2026-05-18T12:31:37.085036+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QHCU57HS77YINARHHTZEAICGBO","json":"https://pith.science/pith/QHCU57HS77YINARHHTZEAICGBO.json","graph_json":"https://pith.science/api/pith-number/QHCU57HS77YINARHHTZEAICGBO/graph.json","events_json":"https://pith.science/api/pith-number/QHCU57HS77YINARHHTZEAICGBO/events.json","paper":"https://pith.science/paper/QHCU57HS"},"agent_actions":{"view_html":"https://pith.science/pith/QHCU57HS77YINARHHTZEAICGBO","download_json":"https://pith.science/pith/QHCU57HS77YINARHHTZEAICGBO.json","view_paper":"https://pith.science/paper/QHCU57HS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.05924&json=true","fetch_graph":"https://pith.science/api/pith-number/QHCU57HS77YINARHHTZEAICGBO/graph.json","fetch_events":"https://pith.science/api/pith-number/QHCU57HS77YINARHHTZEAICGBO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QHCU57HS77YINARHHTZEAICGBO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QHCU57HS77YINARHHTZEAICGBO/action/storage_attestation","attest_author":"https://pith.science/pith/QHCU57HS77YINARHHTZEAICGBO/action/author_attestation","sign_citation":"https://pith.science/pith/QHCU57HS77YINARHHTZEAICGBO/action/citation_signature","submit_replication":"https://pith.science/pith/QHCU57HS77YINARHHTZEAICGBO/action/replication_record"}},"created_at":"2026-05-17T23:58:50.138271+00:00","updated_at":"2026-05-17T23:58:50.138271+00:00"}