{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:YP7ZPJLZGAWXLMGVVV3XEH5NKN","short_pith_number":"pith:YP7ZPJLZ","schema_version":"1.0","canonical_sha256":"c3ff97a579302d75b0d5ad77721fad5365bfc6961fcd1500d81f1292d778bef7","source":{"kind":"arxiv","id":"2403.19360","version":1},"attestation_state":"computed","paper":{"title":"Low Phase Noise, Record-High Power Optical Parametric Oscillator Tunable from 2.7-4.7 {\\mu}m for Metrology Applications","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Michael Leskowschek, Norbert Modsching, Oliver H. Heckl, Thomas S\\\"udmeyer, Valentin J. Wittwer, Vito F. Pecile","submitted_at":"2024-03-28T12:18:50Z","abstract_excerpt":"Within the domain of optical frequency comb systems operating in the mid-infrared, extensive exploration has been undertaken regarding critical parameters such as stabilization, coherence, or spectral tunability. Despite this, certain essential parameters remain inadequately addressed, particularly concerning the light source prerequisites for advanced spectroscopy techniques operating in the 3-5 ${\\mu}$m spectral region. Specifically, the necessity for high simultaneous stability of average power, spectral shape, and temporal properties, alongside requirements for excellent beam quality and h"},"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":"2403.19360","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-28T12:18:50Z","cross_cats_sorted":[],"title_canon_sha256":"6494f1670829a0b5cac02aed243d67d4da8ac778170a997b35ffb3f66b0268df","abstract_canon_sha256":"fcf0b96ef2725c0deab18ac5de6b8074e2b0bd600fa985d61ea0303e924b7e6b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:01:48.166659Z","signature_b64":"+g+l/DOSyMXxKTLH0gurnJjEUMta+3WRsHGuuhmph3/yWGQ5UvyJN32xOXwEVTb2WUl2TaECtLEhLAyCyJrnAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3ff97a579302d75b0d5ad77721fad5365bfc6961fcd1500d81f1292d778bef7","last_reissued_at":"2026-07-05T08:01:48.166193Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:01:48.166193Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Low Phase Noise, Record-High Power Optical Parametric Oscillator Tunable from 2.7-4.7 {\\mu}m for Metrology Applications","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Michael Leskowschek, Norbert Modsching, Oliver H. Heckl, Thomas S\\\"udmeyer, Valentin J. Wittwer, Vito F. Pecile","submitted_at":"2024-03-28T12:18:50Z","abstract_excerpt":"Within the domain of optical frequency comb systems operating in the mid-infrared, extensive exploration has been undertaken regarding critical parameters such as stabilization, coherence, or spectral tunability. Despite this, certain essential parameters remain inadequately addressed, particularly concerning the light source prerequisites for advanced spectroscopy techniques operating in the 3-5 ${\\mu}$m spectral region. Specifically, the necessity for high simultaneous stability of average power, spectral shape, and temporal properties, alongside requirements for excellent beam quality and h"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.19360","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/2403.19360/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2403.19360","created_at":"2026-07-05T08:01:48.166262+00:00"},{"alias_kind":"arxiv_version","alias_value":"2403.19360v1","created_at":"2026-07-05T08:01:48.166262+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.19360","created_at":"2026-07-05T08:01:48.166262+00:00"},{"alias_kind":"pith_short_12","alias_value":"YP7ZPJLZGAWX","created_at":"2026-07-05T08:01:48.166262+00:00"},{"alias_kind":"pith_short_16","alias_value":"YP7ZPJLZGAWXLMGV","created_at":"2026-07-05T08:01:48.166262+00:00"},{"alias_kind":"pith_short_8","alias_value":"YP7ZPJLZ","created_at":"2026-07-05T08:01:48.166262+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/YP7ZPJLZGAWXLMGVVV3XEH5NKN","json":"https://pith.science/pith/YP7ZPJLZGAWXLMGVVV3XEH5NKN.json","graph_json":"https://pith.science/api/pith-number/YP7ZPJLZGAWXLMGVVV3XEH5NKN/graph.json","events_json":"https://pith.science/api/pith-number/YP7ZPJLZGAWXLMGVVV3XEH5NKN/events.json","paper":"https://pith.science/paper/YP7ZPJLZ"},"agent_actions":{"view_html":"https://pith.science/pith/YP7ZPJLZGAWXLMGVVV3XEH5NKN","download_json":"https://pith.science/pith/YP7ZPJLZGAWXLMGVVV3XEH5NKN.json","view_paper":"https://pith.science/paper/YP7ZPJLZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2403.19360&json=true","fetch_graph":"https://pith.science/api/pith-number/YP7ZPJLZGAWXLMGVVV3XEH5NKN/graph.json","fetch_events":"https://pith.science/api/pith-number/YP7ZPJLZGAWXLMGVVV3XEH5NKN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YP7ZPJLZGAWXLMGVVV3XEH5NKN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YP7ZPJLZGAWXLMGVVV3XEH5NKN/action/storage_attestation","attest_author":"https://pith.science/pith/YP7ZPJLZGAWXLMGVVV3XEH5NKN/action/author_attestation","sign_citation":"https://pith.science/pith/YP7ZPJLZGAWXLMGVVV3XEH5NKN/action/citation_signature","submit_replication":"https://pith.science/pith/YP7ZPJLZGAWXLMGVVV3XEH5NKN/action/replication_record"}},"created_at":"2026-07-05T08:01:48.166262+00:00","updated_at":"2026-07-05T08:01:48.166262+00:00"}