{"as_of":"2026-08-17T17:11:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:509e54df003b085f0e2e712ed4f94fe9e4a2221e417fa010db5e7bba30c2274e","coverage":[{"denominator":39,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":39,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T06:08:08.743774Z","state":"measured"},{"denominator":39,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":39,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-17T06:30:58.91139+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/1909.00106/citation-record","integrity":"/paper/1909.00106/integrity","json":"/paper/1909.00106/citation-record.json","paper":"/paper/1909.00106"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.281489Z","title":"Absorption measurements of oxygen between 330 and 1140 nm,","venue":null,"work_id":"5056e240-1924-4a9d-a8b2-4de4782b1f1c","year":1990},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.585705Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:041ace46e777c0163e0867d2bd057525333e0145342f0a6809670c721dbcedbf","observation_id":"1fcf01ed-ceff-4ec1-ab26-dfcc867d5244","resolution":{"observed_at":"2026-08-14T06:08:09.285806Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.269656Z","title":"Properties of Potassium,","venue":null,"work_id":"1d06a7e2-b804-42b1-babe-cc0d1499eaca","year":2010},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.590448Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:baa01d438deb3c245982d15298760749c53d25025ac1f4e6e24c50a1d95a1743","observation_id":"633ccbee-aa05-45e3-9c2a-e794c89d6099","resolution":{"observed_at":"2026-08-14T06:08:09.274004Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.257612Z","title":"Rubidium 87 D Line Data,","venue":null,"work_id":"8c73401e-029c-40b4-9353-6c75894651d3","year":2001},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.594458Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:8c9ecbba7345ce73693b7d128032af4299db59b6c0668d26f3460cd01303d28a","observation_id":"c031a76b-353d-44e4-a39e-81753346fe39","resolution":{"observed_at":"2026-08-14T06:08:09.262050Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.242589Z","title":"Accurate determi- nation of wavenumbers for iodine molecular lines in the red spectral region,","venue":null,"work_id":"4c93bfb5-455b-46bf-8b81-2d5914762e5b","year":1989},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.598715Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:c07d730c29a9064b98f21340057d58242c86b6b751c1e58b408b3e05d88943d0","observation_id":"1b032040-a0ff-4715-b6e6-382c15edc38f","resolution":{"observed_at":"2026-08-14T06:08:09.248341Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1905.11094","last_updated":"2020-01-14T09:21:53Z","snapshot_observed_at":"2026-08-17T13:53:24.818767Z","submitted_at":"2019-05-27T09:58:38Z","title":"Triply magic conditions for microwave transitions of optically trapped alkali-metal atoms","version":3},"cited_work":{"arxiv_id":"1905.11094","doi":null,"metadata_source":"pith","pith_arxiv_id":"1905.11094","snapshot_observed_at":"2026-08-14T06:08:08.794657Z","title":"Triply magic conditions for microwave transitions of optically trapped alkali-metal atoms","venue":"quant-ph","work_id":"49459f30-29f9-44d0-a725-7a2f72bef8a2","year":2019},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.603546Z"},"links":{"cited_paper":"/paper/1905.11094","citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:abc28275d8fdd86c73d5148ee150505ac19cc0ac119b1b85b07a02f5a98e411e","observation_id":"39adca9d-fcf2-4255-97d4-38ae49634b4d","resolution":{"observed_at":"2026-08-14T06:08:08.799179Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.230487Z","title":"Magic-wavelength op- tical dipole trap of cesium and rubidium atoms,","venue":null,"work_id":"276445be-7d09-4a2f-9295-237b65c4a8f5","year":2012},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.608189Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:d7c9d94024cb85081781db8088db248844bf2ac0593fcee6f0dc24e4117a4aa6","observation_id":"7e0826f7-fdeb-4be6-8557-8a844d65641d","resolution":{"observed_at":"2026-08-14T06:08:09.235143Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.216075Z","title":"Implementation of a stable, high-power optical lattice for quantum gas microscopy,","venue":null,"work_id":"56d7f9f1-461b-484c-b4eb-39c90a9b114c","year":2019},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.613127Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:a8afcda8c924f92094f77b46fdb20e8cf33ef5f6c0299c3cfcc9e1eed99ecfe6","observation_id":"753e8026-a329-459d-bf4e-698e12d4bc2a","resolution":{"observed_at":"2026-08-14T06:08:09.221129Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.203749Z","title":"Singly resonant sum-frequency generation of 520-nm laser via a variable input-coupling transmission cavity,","venue":null,"work_id":"c3462be9-f66d-42c0-838d-305dea1315e9","year":2015},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.616797Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:65cf4406b81db4d611875d8d3e2e5b651830417a96a86c66b4e526b30b2a050d","observation_id":"6874eb63-18f2-44c7-b702-475a6b7dc012","resolution":{"observed_at":"2026-08-14T06:08:09.208251Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.191168Z","title":"11 W narrow linewidth laser source at 780nm for laser cooling and manipulation of Rubidium,","venue":null,"work_id":"3d1cc6f8-e603-46d2-90bd-19b5e01e2d2a","year":2012},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.620281Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:05444436ea60a8636b417b0ccd24e79da1ebf8d71d7bbcb45ac279a04c1b9d3a","observation_id":"5b7d40d2-22af-4cbb-89b7-63202df2d6e6","resolution":{"observed_at":"2026-08-14T06:08:09.195720Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.178561Z","title":"A 750-mW, continuous-wave, solid-state laser source at 313 nm for cooling and manipulating trapped 9Be+ ions,","venue":null,"work_id":"45fc77ab-3248-4378-83e6-da78817570cb","year":2011},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.624507Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:5c39cbf60ee2328d9c265bf295807a00f1c63a09e3cf4b0cd7aed6d9f59db56b","observation_id":"1f57496f-2e66-4d34-92b8-21c43904075d","resolution":{"observed_at":"2026-08-14T06:08:09.183501Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.166069Z","title":"A simple 2 W continuous-wave laser system for trapping ultracold metastable helium atoms at the 319.8 nm magic wavelength,","venue":null,"work_id":"472a6caa-cee8-4a24-b75c-5e59f7334a6c","year":2016},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.628262Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:64c725e679a6ee8d81c095a53f8ef026e50318b1f4c0cf39c521ea10fc1b6c11","observation_id":"a57dc5bc-961e-431e-b375-a9b89decfd5b","resolution":{"observed_at":"2026-08-14T06:08:09.170576Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.153200Z","title":"High power single frequency 780nm laser source generated from frequency doubling of a seeded ﬁber ampliﬁer in a cascade of PPLN crystals,","venue":null,"work_id":"2832eb54-8397-4426-9eb9-d058f17f2898","year":2003},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.632085Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:6609fa82070776f584c7646b4b59e94814b8beaa6c414047f28bf29310906d47","observation_id":"cab26821-b27f-412d-be54-2a3bfb244e53","resolution":{"observed_at":"2026-08-14T06:08:09.157786Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.139173Z","title":"Compact and robust laser system for rubidium laser cooling based on the frequency doubling of a ﬁber bench at 1560 nm,","venue":null,"work_id":"f0e9ae22-5f4c-4401-b2dd-b46391faf93a","year":2007},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.636093Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:b298e6450ec8fa1e447a5cc70813e244051f325bb084edb078456a36f9250689","observation_id":"5695e76d-e529-4b03-aece-f32571784aa6","resolution":{"observed_at":"2026-08-14T06:08:09.144424Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.125951Z","title":"Coherent Operations, Entanglement, and Progress To- ward Quantum Search in a Large 2D Array of Neutral Atom Qubits,","venue":null,"work_id":"acff3359-8b5c-444f-8fd8-2762fc38d5bd","year":2015},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.639863Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:ebf826eee7c0a380983004286153b98460b35b76c9bf36ce51f381f0a8adab96","observation_id":"d0ba9357-1216-4fca-acc4-0efb1e44bab6","resolution":{"observed_at":"2026-08-14T06:08:09.131134Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.113531Z","title":"High Average Power Second-Harmonic Generation of a CW Erbium Fiber MOPA,","venue":null,"work_id":"4cf7625a-7f51-4b57-bfbd-08068abba89d","year":2017},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.644033Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:3eb6cca5a2e9311b974819942aa551c3ac9e7d0f39d66e6ba9cb9e550e162b8b","observation_id":"e80c9c81-f824-4080-988f-97511d2699a9","resolution":{"observed_at":"2026-08-14T06:08:09.117841Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1811.03799","last_updated":"2019-11-21T13:15:06Z","snapshot_observed_at":"2026-08-17T08:09:50.791940Z","submitted_at":"2018-11-09T07:14:33Z","title":"Single-Pass Laser Frequency Conversion to 780.2 nm and 852.3 nm Based on PPMgO:LN Bulk Crystals and Diode-Laser-Seeded Fiber Amplifiers","version":4},"cited_work":{"arxiv_id":"1811.03799","doi":null,"metadata_source":"pith","pith_arxiv_id":"1811.03799","snapshot_observed_at":"2026-08-14T06:08:08.774517Z","title":"Single-Pass Laser Frequency Conversion to 780.2 nm and 852.3 nm Based on PPMgO:LN Bulk Crystals and Diode-Laser-Seeded Fiber Amplifiers","venue":"physics.atom-ph","work_id":"f5312b07-3c08-48bb-a6a6-b78c01398359","year":2018},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.647676Z"},"links":{"cited_paper":"/paper/1811.03799","citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:46fa97259ed4d3dae57a68af24bef4f3c28db99365595ee2e10c22d12b21ac0a","observation_id":"41279611-0a4f-40bd-876d-3ec0c1df7aeb","resolution":{"observed_at":"2026-08-14T06:08:08.781847Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.100558Z","title":"Frequency doubled 1534 nm laser system for potassium laser cooling,","venue":null,"work_id":"ec289cf7-2fb7-4dd0-b91e-7a4bab2cbebb","year":2010},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.651654Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:88592391041ef503f38775245ae02364a43c57aab3e982e7f5abeeab33ab869e","observation_id":"1929568a-2f2f-49b5-a647-68f788f546e9","resolution":{"observed_at":"2026-08-14T06:08:09.105228Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.087806Z","title":"High-efﬁciency fre- quency doubling of continuous-wave laser light,","venue":null,"work_id":"4e6124fd-22f8-4ae2-820d-73b6e8d8b8fe","year":2011},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.655670Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:248270a77ce24ad26c29914895e9afd76b291b0d6253938a97fba601bac5b74c","observation_id":"b586aa90-b938-42b5-adfa-4fff52d90953","resolution":{"observed_at":"2026-08-14T06:08:09.092887Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.074118Z","title":"Thermally induced dephasing in periodically poled KTP frequency-doubling crystals,","venue":null,"work_id":"bafe3bb4-1485-40b4-89a4-8c3f3906cd1b","year":2004},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.659383Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:3111f4db20302e70f64cfbcecd77e210cdea352d18a24972e7106a66f1b83a46","observation_id":"04a64b82-63a2-44db-b9d2-a86d967b5419","resolution":{"observed_at":"2026-08-14T06:08:09.079653Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.058787Z","title":"Optimizing non-resonant frequency conversion in periodically poled media,","venue":null,"work_id":"4f520f1a-e53e-4620-a535-9efc5265cf8f","year":2004},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.663087Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:a8471a0315b26b1a05fa34b9ae29b597d0cf6ed2778a5f52f6c370544491cd58","observation_id":"1883fee6-f8f4-49a7-bb68-3223d35e0ce3","resolution":{"observed_at":"2026-08-14T06:08:09.064102Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.045170Z","title":"Thermal inhibi- tion of high-power second-harmonic generation in periodically poled LiNbO3 and LiTaO3 crystals,","venue":null,"work_id":"61dc72ad-f5e1-4433-ab71-e516a01d7bf0","year":2005},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.667330Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:ba91cc23281f5bd2c13f3703e6a4c465c6c52733cde419625562ea34b2a3856f","observation_id":"64b49d28-ce84-413e-9915-b06832003c62","resolution":{"observed_at":"2026-08-14T06:08:09.050101Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.030165Z","title":"Cavity- enhanced generation of 6 W cw second-harmonic power at 532 nm in periodically-poled MgO:LiTaO3,","venue":null,"work_id":"bdb6f934-b9be-4a6e-803b-36b3592a7fc9","year":2010},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.672264Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:6ea6ef457af8a37a5ae6f6711d73acb80bf47617741fb081e8b731a8157d5a36","observation_id":"4c943600-e5a2-4087-9a0f-b0bf036bd497","resolution":{"observed_at":"2026-08-14T06:08:09.035145Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.017470Z","title":"Green-induced infrared absorption in MgO doped LiNbO3,","venue":null,"work_id":"64b08ca4-d69c-4b87-a2c0-7a36eb51011d","year":2001},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.677262Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:0e1383305ac5bbb5c1c42426d77edd02d649150c61402ccf34bd53c94c12bdfc","observation_id":"45e7965c-95f9-4ca8-bcc2-3d589a7895d9","resolution":{"observed_at":"2026-08-14T06:08:09.022125Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:09.004419Z","title":"High-Power CW Green Lasers for Optical Metrology and Their Joint Beneﬁt in Particle Physics Experiments,","venue":null,"work_id":"663331c6-5c77-4a63-9f24-f4f3e69a57c5","year":2011},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.681501Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:c757729b67e0f8f8994a616db37e99b9dbd9c5003af7addfbd0f63ca337d2971","observation_id":"2fd2869a-ac23-4e56-821c-4799bfb02ca8","resolution":{"observed_at":"2026-08-14T06:08:09.008931Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.989787Z","title":"Absolute scale of second-order nonlinear-optical coefﬁcients,","venue":null,"work_id":"52ae6ab8-b721-44cb-a21a-ba0284e85cd0","year":1997},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.685536Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:2e236f28620b20326f71f691b7329b61a6a07bc4816bb9b2ca03930e821e6b7f","observation_id":"59143433-7998-412a-b110-eae95a4777ab","resolution":{"observed_at":"2026-08-14T06:08:08.995504Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.977284Z","title":"High efﬁciency frequency doubling with a passive enhancement cavity,","venue":null,"work_id":"d6c71e8f-f9f6-4684-8d6a-3cf639838377","year":2019},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.690837Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:b4e0a8f7da3a043144d0ebea3f010c9eda55ae53e7fd5f3f43ccca377a827520","observation_id":"2ff2abde-78fc-413d-9a8e-8e75f59d5109","resolution":{"observed_at":"2026-08-14T06:08:08.982114Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.962050Z","title":"Continuous-wave single- frequency 532 nm laser source emitting 130 W into the fundamental transversal mode,","venue":null,"work_id":"d0edd6ab-0bdf-4e22-ad94-4a6ee53285d1","year":2010},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.694815Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:292f577286bce7908b7c581898dfe2cb6b8baa6d062f8615f8e17fa68ae47597","observation_id":"ebba5a36-7cae-4b45-b91f-fbca055e21f5","resolution":{"observed_at":"2026-08-14T06:08:08.968152Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.950535Z","title":"Rydberg-mediated Atomic Ensemble Entanglement and Hy- perﬁne Qubit Detection,","venue":null,"work_id":"11766ca2-74dc-499d-9aef-4b0edcd9b9ee","year":2019},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.699515Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:1e267c76c9ae9cd5b13ab901dea20bb9f89efb45d21b4995b4ccd497e665bbc1","observation_id":"891f39eb-7861-4cba-8bb7-fb906a5af083","resolution":{"observed_at":"2026-08-14T06:08:08.954733Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.938099Z","title":"Laser phase and frequency stabilization using an optical resonator,","venue":null,"work_id":"64bccd17-1fce-43c6-b4be-40f0f261eab7","year":1983},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.704023Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:f18fc5cf313cea3e5336949e5451aebac65a9325c7338b3fa1d57201aadc424a","observation_id":"08889d5b-2a45-4c00-a1d1-884dcebc504b","resolution":{"observed_at":"2026-08-14T06:08:08.942717Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.924557Z","title":"Temperature-tuned 90◦ phase-matching properties of LBO,","venue":null,"work_id":"b8eecd9c-f168-4c9b-9785-b1ecbef57a20","year":1994},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.707782Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:030c4b5c936f5806e258b2137039a996b1fc356dc72b45e7042250a3f8501635","observation_id":"9a2a03fe-d8b5-4a88-b1a8-28468a39b796","resolution":{"observed_at":"2026-08-14T06:08:08.929344Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.910424Z","title":"Laser frequency stabilization by polariza- tion spectroscopy of a reﬂecting reference cavity,","venue":null,"work_id":"70d3449d-675b-4762-8d3e-86f1427cb3a6","year":1980},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.711700Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:eeca68184df43b0e92e5c0814837bc96398acc50a906dd34222fe1acc4bbd8c0","observation_id":"ae4fa339-00bb-4a41-be29-1f1ccef3e07e","resolution":{"observed_at":"2026-08-14T06:08:08.915856Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.899358Z","title":"Stabilization of an optical cavity containing a birefringent element,","venue":null,"work_id":"440ab90e-3af7-4744-a5e1-57b6ce50bb6f","year":1997},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.715467Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:df3d9c567ec40930c087978576e74f553a333ac217a9ab1d1c215b567cc0bc42","observation_id":"cf090ed9-ac4e-48c7-b37e-fe587e91292a","resolution":{"observed_at":"2026-08-14T06:08:08.902858Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.887167Z","title":"Frequency doubling with KNbO3 in an external cavity,","venue":null,"work_id":"881b8c39-1b73-464b-8f16-0ff7f9ceec17","year":1991},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.720054Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:bb8a4410a9a44f778672c7e9f79bc24d8fa21475c16948c31fef8aef14c8b6d6","observation_id":"f8952641-849f-43f0-8454-fb844b5d3221","resolution":{"observed_at":"2026-08-14T06:08:08.891388Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.875374Z","title":"Ultra-narrow linewidth measurement based on Voigt proﬁle ﬁtting,","venue":null,"work_id":"49470ddc-d208-4d56-a7dc-b14539eeee33","year":2015},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.723931Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:6740cf0893cd0c16ef94b98014209cd52cee27ad4bbf96c8fccc67b55099dd17","observation_id":"f8e70706-cca9-4e34-8371-d8db9047a348","resolution":{"observed_at":"2026-08-14T06:08:08.879732Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.863896Z","title":"1/f frequency noise effects on self-heterodyne linewidth measurements,","venue":null,"work_id":"88032658-4a61-4b0e-a4b6-fcd616f3ac3e","year":1991},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.727857Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:b7c54279f6d8a4acfe342810cdb3a013978d49586e62323038a8c2e5bdccccbc","observation_id":"e43f5aa4-56ea-432c-adc3-e33f2bb46da4","resolution":{"observed_at":"2026-08-14T06:08:08.868094Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.850775Z","title":"Cavity-enhanced optical frequency doubler based on transmission-mode Hänsch–Couillaud locking,","venue":null,"work_id":"23b217ec-4da7-45ab-a368-1398254dd152","year":2011},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.732797Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:899feadb5deb737bb14ca7094f434a433511d7c9afce6898f266bf2c13aee01b","observation_id":"9aa30a84-5670-475d-a10d-32313f3b46bf","resolution":{"observed_at":"2026-08-14T06:08:08.855356Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.836123Z","title":"Laser-noise-induced heating in far-off resonance optical traps,","venue":null,"work_id":"b295aeee-06e6-471b-9676-27ab2cb0b81f","year":1997},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.737257Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:bf76d26e64350de514d4e59599ee3ee0a392c68a6baa63ea13517c261b9fa9f6","observation_id":"10734be3-8c9b-4bad-931c-5e6be2c2f0d3","resolution":{"observed_at":"2026-08-14T06:08:08.841128Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.822312Z","title":"Photoacoustic absorption spectrometer for highly transparent dielectrics with parts-per-million sensitivity,","venue":null,"work_id":"7c03e4cf-d717-40b6-b41c-092932c37004","year":2013},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.740633Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:f73a45e9d43b9b1079a2ad47bf8ec3ce9f0880db6010f45d2c43638f97f12711","observation_id":"613c70b9-e835-4763-b5f2-2019ddb15fef","resolution":{"observed_at":"2026-08-14T06:08:08.826889Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T06:08:08.807712Z","title":"75%-Efﬁciency blue gen- eration from an intracavity PPKTP frequency doubler,","venue":null,"work_id":"fdf7bbca-3bd2-42cb-94f5-d9809bc4a265","year":2005},"citing_paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T06:08:08.743774Z"},"links":{"citing_paper":"/paper/1909.00106"},"observation_digest":"sha256:6a4730aca8dc1c01934a1a401eeeafcadfc2bd829418e164acc597d98b76cc87","observation_id":"82b25828-59c2-4845-a558-55a4a3a8ff33","resolution":{"observed_at":"2026-08-14T06:08:08.812675Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"1909.00106","last_updated":"2019-08-31T02:09:33Z","latest_version":1,"primary_category":"physics.optics","snapshot_observed_at":"2026-08-17T12:54:19.611081Z","submitted_at":"2019-08-31T02:09:33Z","title":"Generation of 14.0W of single frequency light at 770 nm by intracavity frequency doubling"},"reference_resolution":{"displayed":39,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":2,"verified_fuzzy":37},"total_outbound_references":39},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"thesis":"As of 17 August 2026, this Paper Citation Record lists 39 of 39 outbound references and 0 inbound Pith citation observations for arXiv:1909.00106."}