{"id":12552,"date":"2026-09-09T16:28:42","date_gmt":"2026-09-09T14:28:42","guid":{"rendered":"https:\/\/soliton-gmbh.de\/?post_type=product&#038;p=12552"},"modified":"2026-09-09T16:41:24","modified_gmt":"2026-09-09T14:41:24","slug":"oe4001-hi-q-laser-rin-analyzer","status":"publish","type":"product","link":"https:\/\/soliton-gmbh.de\/en\/produkt\/oe4001-hi-q-laser-rin-analyzer\/","title":{"rendered":"OE4001 HI-Q\u00ae Laser RIN Analyzer"},"content":{"rendered":"<h2 class=\"PDq2pG_selectionAnchorContainer\" data-section-id=\"6b6spk\" data-start=\"637\" data-end=\"696\">OE4001 \u2013 Precise RIN measurement for low-noise laser sources<\/h2>\n<p data-start=\"698\" data-end=\"1045\">The <strong data-start=\"702\" data-end=\"749\">OE4001 HI-Q\u00ae Laser RIN Analyzer by OEwaves<\/strong> enables the fully automated characterization of the <strong data-start=\"804\" data-end=\"838\">Relative Intensity Noise (RIN)<\/strong> of CW laser sources. The system was specifically developed for applications where even the smallest intensity fluctuations of a laser source can affect measurement accuracy or system performance.<\/p>\n<p data-start=\"1047\" data-end=\"1340\">With a noise floor of up to <strong data-start=\"1080\" data-end=\"1095\">-161 dBc\/Hz<\/strong> allows the characterization of particularly low-noise laser sources. For applications with even higher requirements, a <strong data-start=\"1234\" data-end=\"1287\">XRIN option with a noise floor down to \u2212166 dBc\/Hz<\/strong> available.<\/p>\n<h2 data-section-id=\"1ekf265\" data-start=\"1342\" data-end=\"1394\">Accurately characterize Relative Intensity Noise<\/h2>\n<p data-start=\"1396\" data-end=\"1744\">Relative Intensity Noise describes the temporal fluctuations of the optical output power of a laser relative to its mean power. Especially in highly stable laser systems for metrology, sensor technology, or coherent optical methods, this intensity noise can have a significant impact on the achievable measurement accuracy.<\/p>\n<p data-start=\"1746\" data-end=\"1947\">The OE4001 enables fast and reproducible determination of the RIN, making it suitable for both the development and characterization of laser sources and their quality control.<\/p>\n<h2 data-section-id=\"gtvml2\" data-start=\"1949\" data-end=\"1978\">Wide wavelength range<\/h2>\n<p data-start=\"1980\" data-end=\"2231\">The OE4001 is available in various configurations for <strong data-start=\"2032\" data-end=\"2087\">multiple wavelength bands between 400 and 2200 nm<\/strong> available. This allows a wide variety of CW laser sources from the visible spectral range to the near-infrared spectral range to be investigated.<\/p>\n<p data-start=\"2233\" data-end=\"2509\">Depending on the configuration, measurement bandwidths of <strong data-start=\"2282\" data-end=\"2304\">100 MHz to 40 GHz<\/strong> available. This allows the intensity noise to be analyzed for both conventional low-noise laser sources and demanding high-frequency applications.<\/p>\n<h2 data-section-id=\"1cfcjm4\" data-start=\"2511\" data-end=\"2534\">Typical applications<\/h2>\n<p data-start=\"2536\" data-end=\"2753\">The OE4001 is particularly suited for the characterization of low-noise laser sources in demanding optical systems. Typical application areas of the HI-Q\u00ae test and measurement systems from OEwaves include, among others:<\/p>\n<ul data-start=\"2755\" data-end=\"3019\">\n<li data-section-id=\"gfctlv\" data-start=\"2755\" data-end=\"2811\">Optical sensing and interferometric measurement techniques<\/li>\n<li data-section-id=\"16rwvqy\" data-start=\"2812\" data-end=\"2819\">LIDAR<\/li>\n<li data-section-id=\"pdgkzw\" data-start=\"2820\" data-end=\"2856\">Gas spectroscopy and gas sensing<\/li>\n<li data-section-id=\"1fgkc3y\" data-start=\"2857\" data-end=\"2896\">Optical Metrology and Spectroscopy<\/li>\n<li data-section-id=\"kp7lrr\" data-start=\"2897\" data-end=\"2931\">Coherent optical communication<\/li>\n<li data-section-id=\"8alcj\" data-start=\"2932\" data-end=\"2984\">Development and Characterization of Laser Sources<\/li>\n<li data-section-id=\"1t10m6q\" data-start=\"2985\" data-end=\"3019\">Research and Test &amp; Measurement<\/li>\n<\/ul>\n<p data-start=\"3021\" data-end=\"3204\">OEwaves also cites applications such as acoustic sensing and distributed temperature and strain sensing for its HI-Q\u00ae test and measurement systems.<\/p>\n<h2 data-section-id=\"efx7xe\" data-start=\"3206\" data-end=\"3228\">Advantages of the OE4001<\/h2>\n<ul data-start=\"3230\" data-end=\"3515\">\n<li data-section-id=\"162hcqm\" data-start=\"3230\" data-end=\"3260\">Fully automatic RIN measurement<\/li>\n<li data-section-id=\"b3d5e2\" data-start=\"3261\" data-end=\"3290\">Noise Floor to \u2212161 dBc\/Hz<\/li>\n<li data-section-id=\"b0psu0\" data-start=\"3291\" data-end=\"3324\">Down to -166 dBc\/Hz with XRIN option<\/li>\n<li data-section-id=\"5g0tz4\" data-start=\"3325\" data-end=\"3383\">Various wavelength bands between 400 and 2200 nm<\/li>\n<li data-section-id=\"18cxnib\" data-start=\"3384\" data-end=\"3412\">Measurement bandwidths up to 40 GHz<\/li>\n<li data-section-id=\"h73wnu\" data-start=\"3413\" data-end=\"3461\">Suitable for ultra-low-noise CW laser sources<\/li>\n<li data-section-id=\"1osi662\" data-start=\"3462\" data-end=\"3515\">Fast and reproducible laser characterization<\/li>\n<\/ul>\n<h2 data-section-id=\"q6fq4h\" data-start=\"3517\" data-end=\"3538\">OE4001 by OEwaves<\/h2>\n<p data-start=\"3540\" data-end=\"3911\">The <strong data-start=\"3544\" data-end=\"3579\">OE4001 HI-Q\u00ae Laser RIN Analyzer<\/strong> offers a specialized solution for the precise measurement of the intensity noise of modern CW laser sources. Together with the other HI-Q\u00ae measurement systems from OEwaves, it enables a comprehensive characterization of laser noise, making it particularly suitable for research, development, and demanding optical metrology.<\/p>\n<p data-start=\"3913\" data-end=\"4084\"><strong data-start=\"3913\" data-end=\"4084\">Soliton will assist you in selecting the appropriate OE4001 configuration for your laser source, the required wavelength range, and the desired measurement bandwidth.<\/strong><\/p>","protected":false},"excerpt":{"rendered":"<p><a href=\"https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2023\/08\/oewaves_hlogo_final_CMYK.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-6234\" src=\"https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2023\/08\/oewaves_hlogo_final_CMYK.png\" alt=\"\" width=\"206\" height=\"38\" srcset=\"https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2023\/08\/oewaves_hlogo_final_CMYK.png 1000w, https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2023\/08\/oewaves_hlogo_final_CMYK-600x110.png 600w, https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2023\/08\/oewaves_hlogo_final_CMYK-300x55.png 300w, https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2023\/08\/oewaves_hlogo_final_CMYK-768x141.png 768w, https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2023\/08\/oewaves_hlogo_final_CMYK-18x3.png 18w\" sizes=\"auto, (max-width: 206px) 100vw, 206px\" \/><\/a><\/p>\n<ul>\n<li data-section-id=\"13iry6d\" data-start=\"306\" data-end=\"367\">Fully automatic measurement of Relative Intensity Noise (RIN)<\/li>\n<li data-section-id=\"ox4hrz\" data-start=\"368\" data-end=\"400\">For low-noise CW laser sources<\/li>\n<li data-section-id=\"b3d5e2\" data-start=\"401\" data-end=\"430\">Noise Floor to \u2212161 dBc\/Hz<\/li>\n<li data-section-id=\"1581xoe\" data-start=\"431\" data-end=\"476\">XRIN option with noise floor down to \u2212166 dBc\/Hz<\/li>\n<li data-section-id=\"1d88xhv\" data-start=\"477\" data-end=\"524\">Wavelength ranges between 400 and 2200 nm<\/li>\n<li data-section-id=\"1wnecgg\" data-start=\"525\" data-end=\"575\">Measurement bandwidths up to 40 GHz depending on configuration<\/li>\n<\/ul>","protected":false},"featured_media":12553,"template":"","meta":{"_acf_changed":false,"_uag_custom_page_level_css":"","site-sidebar-layout":"default","site-content-layout":"default","ast-site-content-layout":"default","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","ast-disable-related-posts":"","theme-transparent-header-meta":"default","adv-header-id-meta":"","stick-header-meta":"default","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"set","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center 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