{"id":34437,"date":"2024-05-15T11:40:21","date_gmt":"2024-05-15T09:40:21","guid":{"rendered":"https:\/\/www.eqphotonics.de\/produkt\/aom-3080-1990-for-1060nm\/"},"modified":"2024-05-15T11:40:37","modified_gmt":"2024-05-15T09:40:37","slug":"aom-3080-1990-for-1060nm","status":"publish","type":"product","link":"https:\/\/www.eqphotonics.de\/en\/product\/aom-3080-1990-for-1060nm\/","title":{"rendered":"AOM 3080-1990 for 1060nm"},"content":{"rendered":"<h1 class=\"h2 product_title entry-title\">AOM from G&#038;H<br \/>\n<strong>3080-1990<\/strong><\/h1>\n<p>G&#038;H offers a very wide range of acousto-optical modulators, both based on the in-house manufactured TeO2 for the visible to IR range and on quartz for the UV range as well as for applications requiring high power densities.<\/p>\n<p>TeO2 AOMs are characterised by high efficiency at low RF powers, and are also suitable for unpolarised light in longitudinal mode! The polarisation is preserved!<\/p>\n<div class=\"row ml-0 mr-0 mt-3 bulletdiv\">\n<div class=\"col-md-6 pl-0 mb-3\">\n<h3>Features<\/h3>\n<div class=\"bullets\">TeO2 &#8211; longitudinal Mode<br \/>high efficiency<br \/>very good contrast ratio<br \/>low insertion loss<br \/>diffracting unpolarized laser light<br \/>polarization maintaining<\/div>\n<\/div>\n<div class=\"col-md-6 pl-0 mb-3\">\n<h3>Applications<\/h3>\n<div class=\"bullets\">Heterodyne-interferometry<br \/>printing<br \/>laser tweezer<br \/>material processing<br \/>microscopy<br \/>optical inspection<\/div>\n<\/div>\n<\/div>\n<div class=\"row ml-0 mr-0 mt-3 bulletdivsecond\">\n<div class=\"col-md-6 pl-0 mb-3\">\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>EQ Photonics GmbH has been servicing the wide range of acousto-optical components of the leading manufacturer Gooch and Housego for many years.<\/p>\n<p>Modulators, fibre-coupled modulators, multi-channel modulators, deflectors, Q-switches and tunable filters are manufactured for use in the range from 200nm to over 10\u00b5m!<\/p>\n<p>TeO2, crystalline quartz, germanium, AMTIR and silicon are used as base materials used for these components!<\/p>\n","protected":false},"featured_media":6174,"template":"","meta":{"_acf_changed":false},"product_brand":[],"product_cat":[22012,22257],"product_tag":[],"class_list":{"0":"post-34437","1":"product","2":"type-product","3":"status-publish","4":"has-post-thumbnail","6":"product_cat-acoustooptic","7":"product_cat-aom-acoustooptic","8":"pa_acoustic-mode-longitudinal","9":"pa_acoustic-velocity-in-m-sec-22110","10":"pa_ao-medium-teo2-en","11":"pa_aperture-in-mm-22030","12":"pa_availability-std-lead-times","13":"pa_bandwidth-in-mhz-22832","14":"pa_device-cooling-conduction-cooled","15":"pa_frequency-in-mhz-22895","16":"pa_input-polarization-random","17":"pa_manufacturer-gh","18":"pa_max-rf-power-in-w-22374","19":"pa_model-3080-1990","20":"pa_notes-internal-top-heat-sink","21":"pa_output-polarization-not-specified","22":"pa_part-number-97-03052-01","23":"pa_product-aom","24":"pa_rf-con-sma","25":"pa_separation-angle-in-mrad-22949","26":"pa_typ-risetime-in-ns-159ns-mm","27":"pa_wavelength-in-nm-16708","28":"pa_wavelength-max-in-nm-22948","29":"pa_wavelength-min-in-nm-22419","31":"first","32":"instock","33":"sold-individually","34":"purchasable","35":"product-type-simple"},"acf":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.3 - 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