{"corpus_id":38627355,"paper_sha":"ad544dd98602b0b4bab01f5972443aa601bbffd3","doi":"10.1364/OE.21.018089","arxiv_id":null,"pmid":23938680,"pmcid":null,"mag_id":1986251230,"dblp_id":null,"acl_id":null,"title":"First multi-watt ribbon fiber oscillator in a high order mode.","year":2013,"publication_date":"2013-07-29","venue":"Optics Express","journal":{"name":"Optics express","pages":"\n          18089-96\n        ","volume":"21 15"},"journal_issn":null,"journal_title":null,"publication_types":["JournalArticle"],"pubmed_pub_types":["Journal Article","Research Support, U.S. Gov't, Non-P.H.S."],"s2_fields_of_study":["Materials Science","Physics","Medicine","Engineering"],"reference_count":25,"citation_count":15,"influential_citation_count":1,"is_open_access":false,"arxiv_categories":null,"arxiv_license":null,"arxiv_journal_ref":null,"mesh_headings":[{"d":"Amplifiers, Electronic","mj":true,"ui":"D000669"},{"d":"Computer-Aided Design","mj":false,"ui":"D017076"},{"d":"Energy Transfer","mj":false,"ui":"D004735"},{"d":"Equipment Design","mj":false,"ui":"D004867"},{"d":"Equipment Failure Analysis","mj":false,"ui":"D019544"},{"d":"Fiber Optic Technology","mj":false,"qs":[{"q":"instrumentation","mj":true,"ui":"Q000295"}],"ui":"D005336"},{"d":"Light","mj":false,"ui":"D008027"},{"d":"Oscillometry","mj":false,"qs":[{"q":"instrumentation","mj":true,"ui":"Q000295"}],"ui":"D009991"},{"d":"Scattering, Radiation","mj":false,"ui":"D012542"}],"chemicals":null,"comments_corrections":null,"source_flags":5,"s2_open_access_pdf_url":null,"s2_open_access_landing_url":null,"s2_open_access_license":null,"s2_open_access_status":null,"pmc_open_access_pdf_url":null,"pmc_open_access_landing_url":null,"pmc_open_access_license":null,"pmc_open_access_status":null,"unpaywall_open_access_pdf_url":null,"unpaywall_open_access_landing_url":null,"unpaywall_open_access_license":null,"unpaywall_open_access_status":null,"abstract":"Optical fibers in the ribbon geometry have the potential to reach powers well above the maximum anticipated power of a circular core fiber. In this paper we report the first doped silica high order mode ribbon fiber oscillator, with multimode power above 40 W with 71% slope efficiency and power in a single high order mode above 5 W with 44% slope efficiency.","claims":[{"public_id":"cl_468494fafd6af7c6f9175a85feeba45e","status":"active","text":"A doped silica high order mode ribbon fiber oscillator is demonstrated for the first time.","confidence":0.98,"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/claims/cl_468494fafd6af7c6f9175a85feeba45e"},{"public_id":"cl_fa5c807a96b7de0d31773d603f0fe5fd","status":"active","text":"Multimode output power exceeds 40 W with 71% slope efficiency.","confidence":0.97,"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/claims/cl_fa5c807a96b7de0d31773d603f0fe5fd"},{"public_id":"cl_9f15937471dc3215bae059eb17d83e78","status":"active","text":"Single high order mode output power exceeds 5 W with 44% slope efficiency.","confidence":0.97,"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/claims/cl_9f15937471dc3215bae059eb17d83e78"}],"concepts":[{"public_id":"co_2d9c0e22a733c5a2c8edceecd7ac6be6","status":"active","name":"multimode power","description":"The total optical output power measured while multiple modes are present.","types":["measurement"],"aliases":[],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_2d9c0e22a733c5a2c8edceecd7ac6be6"},{"public_id":"co_54bde701decd531b7e7dcdc37fe9c1f2","status":"active","name":"high order mode ribbon fiber","description":"A ribbon-geometry optical fiber designed to support propagation in higher-order modes.","types":["optical fiber","waveguide"],"aliases":["ribbon fiber"],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_54bde701decd531b7e7dcdc37fe9c1f2"},{"public_id":"co_6d6baacd61574a0b93117eb677814855","status":"active","name":"doped silica high order mode ribbon fiber oscillator","description":"A laser oscillator built from doped silica ribbon fiber that operates in a high order optical mode.","types":["laser oscillator","fiber laser"],"aliases":["high order mode ribbon fiber oscillator"],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_6d6baacd61574a0b93117eb677814855"},{"public_id":"co_82c8a2e07c3394acab641db474bda041","status":"active","name":"single high order mode power","description":"The optical output power carried by one selected high order mode.","types":["measurement"],"aliases":[],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_82c8a2e07c3394acab641db474bda041"},{"public_id":"co_d71e8832da117aa7dbdc2814777fd447","status":"active","name":"slope efficiency","description":"The rate at which output power increases with increasing pump power.","types":["performance metric"],"aliases":[],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_d71e8832da117aa7dbdc2814777fd447"},{"public_id":"co_f11d508b42f017eacfd03de66bfebd81","status":"active","name":"high order mode","description":"An optical mode with a field distribution above the fundamental mode order.","types":["optical mode"],"aliases":["HOM"],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_f11d508b42f017eacfd03de66bfebd81"}],"external_ids":{"DOI":"10.1364/OE.21.018089","ArXiv":null,"PubMed":23938680,"PubMedCentral":null,"MAG":1986251230,"DBLP":null,"ACL":null},"open_access":{"is_open_access":false,"pdf_url":null,"landing_url":"https://sah.borca.ai/papers/38627355","source":null,"pdf_url_source":null,"license":null,"reason":"pdf_url_not_indexed"},"reference_availability":{"status":"available","references_indexed":true,"full_text_available":false,"full_text_source":null,"count_basis":"semantic_scholar_metadata","extraction_status":"not_applicable","reason":null},"source":{"provider":"episteme2","base_corpus":"semantic_scholar_dump","freshness_mode":"unknown","basis":["semantic_scholar_metadata","postgres_metadata"],"limits":["paper metadata is based on indexed upstream scholarly datasets","claims and concepts are available only for extracted papers","absence of claims or concepts means no extracted graph data is available in this response"],"status":"available","degraded":false,"degraded_reasons":[],"diagnostics":{"status":"available","degraded":false,"degraded_reasons":[],"metadata_status":"available","graph_status":"available","abstract_status":"available"},"source_flags":5},"paper_id":632322,"paper_uid":"f341bb5a-54c8-4760-9c8e-f10a7819d3f4","canonical_identity":{"paper_id":632322,"paper_uid":"f341bb5a-54c8-4760-9c8e-f10a7819d3f4","identity_status":"available","lookup_basis":"semantic_scholar_external_id","compatibility_path":"corpus_id"},"url":"https://sah.borca.ai/papers/38627355"}