{"id":1002,"date":"2021-07-27T13:35:34","date_gmt":"2021-07-27T05:35:34","guid":{"rendered":"https:\/\/kelly.anjun.com.tw\/?page_id=1002"},"modified":"2021-11-01T15:52:46","modified_gmt":"2021-11-01T07:52:46","slug":"automated-monochromator-spectrograph-2","status":"publish","type":"page","link":"https:\/\/www.anjun.com.tw\/en\/%e9%9b%b7%e5%b0%84\/%e9%9b%b7%e5%b0%84%e9%80%b1%e9%82%8a%e8%a8%ad%e5%82%99%e9%8a%b7%e5%94%ae\/solar-ls%e9%9b%b7%e5%b0%84\/spectral-instruments\/monochromators-spectrographs\/automated-monochromator-spectrograph-2\/","title":{"rendered":"AUTOMATED MONOCHROMATOR-SPECTROGRAPH"},"content":{"rendered":"<div data-elementor-type=\"wp-page\" data-elementor-id=\"1002\" class=\"elementor elementor-1002\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-422f511 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"422f511\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-177eab3\" data-id=\"177eab3\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-6c37767 elementor-widget elementor-widget-heading\" data-id=\"6c37767\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Model M266<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-9460ea0 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"9460ea0\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-b0c4abf\" data-id=\"b0c4abf\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-61ce848 elementor-tabs-view-horizontal elementor-widget elementor-widget-tabs\" data-id=\"61ce848\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"tabs.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-tabs\">\n\t\t\t<div class=\"elementor-tabs-wrapper\" role=\"tablist\" >\n\t\t\t\t\t\t\t\t\t<div id=\"elementor-tab-title-1021\" class=\"elementor-tab-title elementor-tab-desktop-title\" aria-selected=\"true\" data-tab=\"1\" role=\"tab\" tabindex=\"0\" aria-controls=\"elementor-tab-content-1021\" aria-expanded=\"false\">DESCRIPTION<\/div>\n\t\t\t\t\t\t\t\t\t<div id=\"elementor-tab-title-1022\" class=\"elementor-tab-title elementor-tab-desktop-title\" aria-selected=\"false\" data-tab=\"2\" role=\"tab\" tabindex=\"-1\" aria-controls=\"elementor-tab-content-1022\" aria-expanded=\"false\">SPECIFICATIONS<\/div>\n\t\t\t\t\t\t\t\t\t<div id=\"elementor-tab-title-1023\" class=\"elementor-tab-title elementor-tab-desktop-title\" aria-selected=\"false\" data-tab=\"3\" role=\"tab\" tabindex=\"-1\" aria-controls=\"elementor-tab-content-1023\" aria-expanded=\"false\">OPTIONS & ACCESSORIES<\/div>\n\t\t\t\t\t\t\t\t\t<div id=\"elementor-tab-title-1024\" class=\"elementor-tab-title elementor-tab-desktop-title\" aria-selected=\"false\" data-tab=\"4\" role=\"tab\" tabindex=\"-1\" aria-controls=\"elementor-tab-content-1024\" aria-expanded=\"false\">OPTICAL BENCH FEATURES<\/div>\n\t\t\t\t\t\t\t<\/div>\n\t\t\t<div class=\"elementor-tabs-content-wrapper\" role=\"tablist\" aria-orientation=\"vertical\">\n\t\t\t\t\t\t\t\t\t<div class=\"elementor-tab-title elementor-tab-mobile-title\" aria-selected=\"true\" data-tab=\"1\" role=\"tab\" tabindex=\"0\" aria-controls=\"elementor-tab-content-1021\" aria-expanded=\"false\">DESCRIPTION<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1021\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"1\" role=\"tabpanel\" aria-labelledby=\"elementor-tab-title-1021\" tabindex=\"0\" hidden=\"false\"><h4 class=\"title text-left\"><span style=\"color: #000000;\">FEATURES<\/span><\/h4><div class=\"text\"><p><span style=\"color: #000000;\">Monochromator M266 is our general-purpose high-aperture instrument with high line quality and low stray light performance, featuring 284mm focus and 30x10mm flat field.<\/span><\/p><ul><li><p><span style=\"color: #000000;\">HIGH APERTURE RATIO (F=1:3.8)<\/span><\/p><\/li><li><p><span style=\"color: #000000;\">TWO OUTPUT PORTS<\/span><\/p><\/li><li><p><span style=\"color: #000000;\">THE M266I VERSION (IMAGING)<\/span><\/p><\/li><li><p><span style=\"color: #000000;\">M266 IS COMPLETELY AUTOMATED<\/span><\/p><\/li><\/ul><h2><span style=\"color: #000000;\">DESCRIPTION<\/span><\/h2><p><span style=\"color: #000000;\"><img decoding=\"async\" src=\"https:\/\/www.anjun.com.tw\/wp-content\/uploads\/2019\/01\/M266_01-300x180.jpg\" \/><img decoding=\"async\" src=\"https:\/\/www.anjun.com.tw\/wp-content\/uploads\/2019\/01\/M266_02-300x180.jpg\" \/><\/span><\/p><p><span style=\"color: #000000;\"><strong>High aperture ratio (F=1:3.8)<\/strong>,\u00a0<strong>low stray light<\/strong>\u00a0and\u00a0<strong>perfect line quality<\/strong>\u00a0enable successful use of the M266 in a wide range of applications.<\/span><\/p><p><span style=\"color: #000000;\"><strong>Two output ports<\/strong>\u00a0allow connecting to the M266 either two exit slits, exit slit\/detector or two detectors concurrently.<\/span><\/p><p><span style=\"color: #000000;\"><strong>The M266i version (Imaging)<\/strong>\u00a0features an astigmatism compensator for both output ports, thus promoting the use of the M266 with matrix detectors in the multi-channel spectroscopy, not only in the binning mode, but also in the 2D-image mode.<\/span><\/p><p><span style=\"color: #000000;\"><strong>M266 is completely automated<\/strong>. Spectrum scanning along wavelengths, change of gratings and order separating filters, adjustment of slit width and selection of an output port are performed automatically, guided by the intelligent and easy-to-use software.<\/span><\/p><p><span style=\"color: #000000;\"><strong>An automatic shutter<\/strong>\u00a0provides for automatic background (dark current) subtraction, along with detector protection against excessive illumination from the light source.<\/span><\/p><p><span style=\"color: #000000;\"><strong>The SolarLS.LAB software<\/strong>\u00a0provides automated control over the monochrometer M266 and its detectors. It allows stitching spectra obtained by several diffraction grating scans in order to get a panoramic spectrum. Many possibilities of spectra processing and analysis are provided as well.<\/span><\/p><p><span style=\"color: #000000;\">At your request,\u00a0<strong>DLL andor LabView drivers<\/strong>\u00a0are supplied with the M266 for controlling the instrument via the customised software or LabView.<\/span><\/p><p><span style=\"color: #000000;\">APPLICATIONS<\/span><\/p><ul><li><p><span style=\"color: #000000;\">Emission, Fluorescence and Raman Spectroscopy<\/span><\/p><\/li><li><p><span style=\"color: #000000;\">Multi-Channel Spectroscopy<\/span><\/p><\/li><li><p><span style=\"color: #000000;\">Absorption, Reflection and Transmission<\/span><\/p><\/li><li><p><span style=\"color: #000000;\">Measurements<\/span><\/p><\/li><li><p><span style=\"color: #000000;\">Analytical Tasks from UV to IR<\/span><\/p><\/li><\/ul><h2><span style=\"color: #000000;\">INSTRUMENT CONFIGURATION<\/span><\/h2><p><span style=\"color: #000000;\">The M266 comprises one input port and two output ports. The input port may hold either a standard entrance slit, or a crossed entrance slit (optionally). All the spectral slits are automated; their width is adjusted by the instrument software. The slit design also contains a microscrew, which provides the possibility to manually adjust the opening width of the knives.<\/span><\/p><p><span style=\"color: #000000;\">Depending on modification, the M266 may contain either a turret with four diffraction gratings, or one grating in the holder.<\/span><\/p><table border=\"1\"><thead><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">MODIFICATION<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">COMPONENTS<\/span><\/td><\/tr><\/thead><tbody><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">M266-IV<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">The standard optics and the turret with 4 diffraction gratings<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">M266i-IV<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">The Imaging optics (astigmatism compensator) and the turret with 4 diffraction gratings<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">M266-I<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">The standard optics and one diffraction grating<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">M266i-I<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">The Imaging optics (astigmatism compensator) and one diffraction grating<\/span><\/td><\/tr><\/tbody><\/table><p><span style=\"color: #000000;\">The standard optics comprises spherical and flat mirrors with Al+MgF2 coating optimised for high UV efficiency. Optionally the device may contain optics with Al+SiO2 or gold coating for high efficiency in the infrared spectral range.<\/span><\/p><p><span style=\"color: #000000;\"><img decoding=\"async\" class=\"aligncenter\" src=\"https:\/\/www.anjun.com.tw\/wp-content\/uploads\/2019\/01\/m266_dim-300x204.png\" \/><\/span><\/p><p><span style=\"color: #000000;\">The M266 output ports may hold either two exit slits, or one exit slit and detector, or two detectors concurrently.<\/span><\/p><p><span style=\"color: #000000;\">Direct (axial) and lateral (radial) output ports operate alternately. Switching between the output ports is effected by the software with the use of the swinging mirror, which in its operating position directs light to the lateral (radial) output port. The instrument is also available with one output (axial) port. If the radial output port is not used, it is plugged.<\/span><\/p><p><span style=\"color: #000000;\">The M266 exit slit has 4 mounting holes M2.5 that allow you fixing your own detector to the slit housing, if necessary. Location of the mounting holes is shown in the figure below.<\/span><\/p><p><span style=\"color: #000000;\"><img decoding=\"async\" class=\"aligncenter\" src=\"https:\/\/www.anjun.com.tw\/wp-content\/uploads\/2019\/01\/m266_slit_en-300x203.png\" \/><\/span><\/p><p><span style=\"color: #000000;\"><em><strong>Note: To avoid a breakdown of the slit mechanism it is prohibited to fix any units weighing more than 1kg to the slit housing.<\/strong><\/em><\/span><\/p><\/div><p><style type=\"text\/css\">\n<!-- table{ border-collapse:separate; collapse;border:1px solid black; } td{ collapse;border:1px solid black; } --><br \/><\/style><\/p><\/div>\n\t\t\t\t\t\t\t\t\t<div class=\"elementor-tab-title elementor-tab-mobile-title\" aria-selected=\"false\" data-tab=\"2\" role=\"tab\" tabindex=\"-1\" aria-controls=\"elementor-tab-content-1022\" aria-expanded=\"false\">SPECIFICATIONS<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1022\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"2\" role=\"tabpanel\" aria-labelledby=\"elementor-tab-title-1022\" tabindex=\"0\" hidden=\"hidden\"><h4><span style=\"color: #000000;\">SPECIFICATIONS<\/span><\/h4><table border=\"1\" width=\"100%\"><thead><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>OPTICAL BENCH<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><p><span style=\"color: #000000;\">OPTIMIZED CZERNY-TURNER WITH ONE INPUT AND TWO OUTPUTS<\/span><\/p><\/td><\/tr><\/thead><tbody><tr><td style=\"text-align: center;\" width=\"28%\"><p><span style=\"color: #000000;\"><strong>Spectral range<\/strong><\/span><\/p><p><span style=\"color: #000000;\"><strong>\u00a0<\/strong><\/span><\/p><\/td><td colspan=\"4\" width=\"71%\"><p style=\"text-align: center;\"><span style=\"color: #000000;\">\u2014 typical 180 \u2013 3600 nm (see the specifications below),<\/span><\/p><p style=\"text-align: center;\"><span style=\"color: #000000;\">\u2014 extended up to 40 \u00b5m (upon request)<\/span><\/p><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>F\/Number<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">1 : 3.8<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>Focal length, mm<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">284<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>Flat field, mm<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">30 x 10<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>Imaging<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">Option. Available for the both output ports simultaneously.<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>Gratings<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><p><span style=\"color: #000000;\">50x50x10mm, one grating or a turret with 4 gratings from the list below<sup>1)<\/sup>.<\/span><\/p><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u00a0\u2014 grooves\/mm<sup>1)<\/sup><\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">1800<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">1200<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">600<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">300<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 reciprocal linear dispersion (average), nm\/mm<sup>\u00a02)<\/sup><\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">2.12<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">3.18<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">6.37<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">12.64<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 blazing wavelength, nm<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">270<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">400<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">750<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">2000<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 spectral range, nm<sup>\u00a03)<\/sup><\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">180-600<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">265-900<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">500-1500<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">1330-3600<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 multichannel array bandpass, (average), nm<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">51\u00a0<sup>4)<\/sup><\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">76\u00a0<sup>4)<\/sup><\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">150\u00a0<sup>4)<\/sup><\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">160\u00a0<sup>5)<\/sup><\/span><\/td><\/tr><tr><td style=\"text-align: center;\" rowspan=\"2\" width=\"28%\"><span style=\"color: #000000;\">\u2014 resolution (average), nm<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">&lt;0.15<sup>4)<\/sup><\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">&lt;0.22<sup>4)<\/sup><\/span><\/td><td style=\"text-align: center;\" rowspan=\"2\" width=\"17%\"><p><span style=\"color: #000000;\">&lt;0.45\u00a0<sup>4)<\/sup><\/span><\/p><p><span style=\"color: #000000;\">0.2<sup>6)<\/sup><\/span><\/p><\/td><td style=\"text-align: center;\" rowspan=\"2\" width=\"17%\"><span style=\"color: #000000;\">&lt;0.94<sup>5)<\/sup><\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">0.07<sup>6)<\/sup><\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">0.1<sup>6)<\/sup><\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Wavelength accuracy, nm<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">\u00b10.067<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">\u00b10.1<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">\u00b10.2<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">\u00b10.4<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Wavelength reproducibility, nm<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">\u00b10.017<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">\u00b10.025<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">\u00b10.05<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">\u00b10.1<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Step of grating rotation, nm<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">0.009<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">0.013<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">0.026<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">0.05<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Scanning speed, nm\/s<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">16.7<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">25<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">50<\/span><\/td><td style=\"text-align: center;\" width=\"17%\"><span style=\"color: #000000;\">100<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>Entrance\/exit slits<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">Automatic and manual adjustment<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Slit width, mm<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">0 \u2014 2<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Slit height, mm<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">12<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Parallelism, \u00b5m<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">+\/- 1<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Micrometer reading accuracy, \u00b5m<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">+\/- 1<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Step size, \u00b5m<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">0.5<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Precision, \u00b5m<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">+\/- 10<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>Filter wheel<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">Automatic switching<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Max number of filters<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">8<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Standard number of filters<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">5<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Filter size, mm<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">20<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\">\u2014 Light aperture, mm<\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">18<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>Integrated shutter<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">Computer controlled, serves for dark signal measuring<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>Computer interface<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">High-Speed USB<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"28%\"><span style=\"color: #000000;\"><strong>Dimensions and Weight<\/strong><\/span><\/td><td style=\"text-align: center;\" colspan=\"4\" width=\"71%\"><span style=\"color: #000000;\">252 \u0445 213 mm, 23.5 kg<\/span><\/td><\/tr><\/tbody><\/table><p><em><span style=\"color: #000000;\">1) Upon your request, diffraction gratings with another grooves quantity\/blazing angle can be used.<\/span><\/em><\/p><p><em><span style=\"color: #000000;\">2) Reciprocal linear dispersion is indicated for blazing wavelength<\/span><\/em><\/p><p><em><span style=\"color: #000000;\">3) Wavelength range for which diffraction efficiency exceeds 40%<\/span><\/em><\/p><p><em><span style=\"color: #000000;\">4) For detector with 24\u00a0\u00b5m pixel size and 5 mm active area<\/span><\/em><\/p><p><em><span style=\"color: #000000;\">5) For detector with 25\u00a0\u00b5m pixel size and 8 mm active area<\/span><\/em><\/p><p><em><span style=\"color: #000000;\">6) For detector with 8\u00a0\u00b5m pixel size and 1 mm active area<\/span><\/em><\/p><\/div>\n\t\t\t\t\t\t\t\t\t<div class=\"elementor-tab-title elementor-tab-mobile-title\" aria-selected=\"false\" data-tab=\"3\" role=\"tab\" tabindex=\"-1\" aria-controls=\"elementor-tab-content-1023\" aria-expanded=\"false\">OPTIONS & ACCESSORIES<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1023\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"3\" role=\"tabpanel\" aria-labelledby=\"elementor-tab-title-1023\" tabindex=\"0\" hidden=\"hidden\"><h4 class=\"title-tab title text-left\"><span style=\"color: #000000;\">OPTIONS &amp; ACCESSORIES<\/span><\/h4><p><span style=\"color: #000000;\">The M266 monochromator-spectrograph has a wide range of\u00a0<strong>options and accessories<\/strong>\u00a0that provide efficient light collection from the sample located at a finite distance and at infinity, delivering light to the monochromator with and without an optical fiber, effective aperture matching of the optical fiber and monochromator.<\/span><\/p><p><span style=\"color: #000000;\">Order Separating Filters Wheels<\/span><\/p><p><span style=\"color: #000000;\">Aperture Matching Adapters<\/span><\/p><p><span style=\"color: #000000;\">Condensers for collecting light into the fiber<\/span><\/p><p><span style=\"color: #000000;\">Condensers for collecting light into the monochromator<\/span><\/p><p><span style=\"color: #000000;\">Crossed Entrance Slit (optionally installed instead of the Standard Entrance Slit)<\/span><\/p><p><span style=\"color: #000000;\">Optical Fibers<\/span><\/p><p><span style=\"color: #000000;\">Adapters for attaching CCD detectors<\/span><\/p><p><span style=\"color: #000000;\">CCD detectors<\/span><\/p><p><span style=\"color: #000000;\">Cassegrain lenses<\/span><\/p><p><span style=\"color: #000000;\">All exit slits are equipped with precision focusing devices; and detector adapters allow easy detector focusing. The detector adapter of the long-focus M833 monochromator-spectrograph allows changing the slope of detector plane relative to the optical bench.<\/span><\/p><p><span style=\"color: #000000;\">Cassegrain lenses\u00a0allow collecting light from objects located at a distance of 3.5m to infinity.<\/span><\/p><p><span style=\"color: #000000;\">Adapters\u00a0PS-2\u00a0and\u00a0PS-3\u00a0are designed for the collection of light from a closely located sample and its effective input into an optical fiber. PS-2 features high transmittance in the UV range, while PS-3 has the possibility of installing an edge filter.<\/span><\/p><p><span style=\"color: #000000;\"><strong><em>Contact a SOLAR LS specialist to select the complete set of your monochromator-spectrograph that meets the requirements for your instrument complex in the best way.<\/em><\/strong><\/span><\/p><p><span style=\"color: #000000;\">MULTI-CHANNEL CCD DETECTORS<\/span><\/p><table border=\"1\" width=\"100%\"><thead><tr><td style=\"text-align: center;\" colspan=\"2\"><span style=\"color: #000000;\"><strong>MULTICHANNEL CCD DETECTORS BY ANDOR TECHNOLOGY TM<\/strong><\/span><\/td><\/tr><\/thead><tbody><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>iVac Series, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">DR 324B-FI model, front-illuminated CCD sensor, UltraVacTM thermo-electric cooling down to -60\u00b0C, spectral range 400-1000nm, 1650*200pixels, pixel size 16*16\u00b5m, image area 26.4mm * 3.2mm, 16 bits digitisation<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" rowspan=\"2\"><span style=\"color: #000000;\"><strong>iDus Series, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">DV 401A-BV model, back-illuminated CCD sensor, UltraVacTM thermo-electric cooling down to -70\u00b0C, spectral range 200-1100nm, 1024*127pixels, pixel size 26*26\u00b5m, image area 26.6mm * 3.6mm, 16 bits digitisation<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">DU 401A-BV model, back-illuminated CCD sensor, UltraVacTM thermo-electric cooling down to -100\u00b0C, spectral range 200-1100nm, 1024*127pixels, pixel size 26*26\u00b5m, image area 26.6mm * 3.6mm, 16 bits digitisation.<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" rowspan=\"2\"><span style=\"color: #000000;\"><strong>Newton Series, EMCCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">DU970P-FI model (*), front-illuminated EMCCD sensor, UltraVacTM thermo-electric cooling down to -100\u00b0C, spectral range 400-1000nm, 1600*200pixels, pixel size 16*16\u00b5m, dual output amplifier, crop mode, Variable readout speed up to 3MHz, 16 bits digitisation.<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">DU970P-BV model (*), back-illuminated EMCCD sensor, UltraVacTM thermo-electric cooling down to -100\u00b0C, spectral range 200-1000nm, 1600*200pixels, pixel size 16*16\u00b5m, dual output amplifier, crop mode, Variable readout speed up to 3MHz, 16 bits digitisation<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>iStar Series, Gated iCCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">DH320T-25U-03 model (*), Ultra Fast Gated Intensified CCD Camera, spectral range 200-900nm, 124*256 CCD 100% Fill Factor, 25mm tube, Gen2 Multialkali S20 Photocathode, P43 phosphor Multi-Mhz Readout Speeds, Integrated Digital Delay Generator, 3 ns Crop Mode sensor, Photocathode dry gas purge port, USB data interface.<\/span><\/td><\/tr><\/tbody><\/table><p><span style=\"color: #000000;\"><em>(*) other models are supplied upon request<\/em><\/span><\/p><table border=\"1\"><thead><tr><td style=\"text-align: center;\" colspan=\"2\"><span style=\"color: #000000;\"><strong>TWO-DIMENSIONAL HAMAMATSU ARRAYS FOR THE 200-1100NM RANGE<\/strong><\/span><\/td><\/tr><\/thead><tbody><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>UC-16H7306, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S7030-1006 sensor, non-cooled, spectral range 200-1100nm, 1024\u00d764 pixels, pixel size 24\u00d724\u00b5m, image area 24.6\u00d71.4mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>UC-16H7307, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S7030-1007 sensor, non-cooled, spectral range 200-1100nm, 1024\u00d7128 pixels, pixel size 24\u00d724\u00b5m, image area 24.6\u00d72.9mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>UC-16H7316, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S7031-1006 back-illuminated sensor, TE cooling \u201310\u00b0C, spectral range 200-1100nm, 1024\u00d764 pixels, pixel size 24\u00d724\u00b5m, image area 24.6\u00d71.4mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>UC-16H7317, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S7031-1007 back-illuminated sensor, TE cooling \u201310\u00b0C, spectral range 200-1100nm, 1024\u00d7128 pixels, pixel size 24\u00d724\u00b5m, image area 24.6\u00d72.9mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>UC-16H7318, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S7031-1008 back-illuminated sensor, TE cooling \u201310\u00b0C, spectral range 200-1100nm, 1024\u00d7256 pixels, pixel size 24\u00d724 \u00b5m, image area 24.6 x 6.1mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>U2C-16H10426, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S10420-1106-01 back-illuminated sensor, non-cooled, spectral range 200-1100nm, 2068\u044570 pixels, pixel size 14\u044514 \u00b5m, image area 28.672\u04450.896mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>U2C-16H<\/strong><strong>11516<\/strong><strong>, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S11510-1106 back-illuminated sensor, non-cooled, spectral range 200-1100nm, 2068\u044570 pixels, pixel size 14\u044514 \u00b5m, image area 28,672\u04450,896mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>U2C-16H11850, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S11850 back-illuminated sensor, TE cooling 5\u00b0\u0421, , spectral range 200-1200nm, 2068\u044570 pixels, pixel size 14\u044514 \u00b5m, image area 28,672\u04450,896mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>U2C-16H<\/strong><strong>101409<\/strong><strong>, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S10140-1109 back-illuminated sensor, non-cooled, , spectral range 200-1100nm, 2068\u044570 pixels, pixel size 14\u044514 \u00b5m, image area 28,672\u04450,896mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\"><strong>U2C-16H<\/strong><strong>101419<\/strong><strong>, Spectroscopic CCD<\/strong><\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">S10141-1109 back-illuminated sensor, TE cooling -10\u00b0C, , spectral range 200-1200nm, 2068\u0445512 pixels, pixel size 12\u044512 \u00b5m, image area 24,576\u04456,072mm, 16 bit digitization<\/span><\/td><\/tr><\/tbody><\/table><table border=\"1\"><thead><tr><td style=\"text-align: center;\" colspan=\"2\" width=\"652\"><span style=\"color: #000000;\"><strong>LINEAR INGAAS HAMAMATSU SENSORS FOR NIR-RANGE 900-1700NM (UP TO 2600NM)<\/strong><\/span><\/td><\/tr><\/thead><tbody><tr><td style=\"text-align: center;\" width=\"151\"><span style=\"color: #000000;\"><strong>UC-16H904, InGaAs sensor<\/strong><\/span><\/td><td style=\"text-align: center;\" width=\"500\"><span style=\"color: #000000;\">G9204-512D image sensor, spectral range 0.9-1.7\u00b5m, non-cooled, 512 pixels, pixel size 25\u00d7500\u00b5m, image area 12.8\u00d70.5mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"151\"><span style=\"color: #000000;\"><strong>UC-16H912, InGaAs sensor<\/strong><\/span><\/td><td style=\"text-align: center;\" width=\"500\"><span style=\"color: #000000;\">G9212-512S image sensor, InGaAs, spectral range 0.9-1.7\u00b5m, TE cooling \u201310\u00b0C, 512 pixels, pixel size 25\u00d7250\u00b5m, image area 12.8\u00d70.25mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"151\"><span style=\"color: #000000;\"><strong>UC-16H914, InGaAs sensor<\/strong><\/span><\/td><td style=\"text-align: center;\" width=\"500\"><span style=\"color: #000000;\">G9214-512S image sensor, InGaAs, spectral range 0.9-1.7\u00b5m, TE cooling \u201310\u00b0C, 512 pixels, pixel size 25\u00d7500\u00b5m, image area 12.8\u00d70.5mm, 16 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"151\"><span style=\"color: #000000;\"><strong>UC-16H908, InGaAs sensor<\/strong><\/span><\/td><td style=\"text-align: center;\" width=\"500\"><span style=\"color: #000000;\">G9208-256W image sensor, InGaAs, spectral range 0.9-2.6\u00b5m, TE cooling \u20132C0\u00b0C, 256 pixels, pixel size 50\u00d7250\u00b5m, image area 12.8\u00d70.25mm, 16 bit digitization<\/span><\/td><\/tr><\/tbody><\/table><table border=\"1\"><thead><tr><td style=\"text-align: center;\" colspan=\"2\" width=\"652\"><span style=\"color: #000000;\"><strong>LINEAR NON-COOLED SENSORS FOR THE 200-1100NM RANGE<\/strong><\/span><\/td><\/tr><\/thead><tbody><tr><td style=\"text-align: center;\" width=\"151\"><span style=\"color: #000000;\"><strong>UC-12T3<\/strong><\/span><\/td><td style=\"text-align: center;\" width=\"500\"><span style=\"color: #000000;\">TCD1304 image sensor, spectral range 190-1100nm, non-cooled, 3648 pixels, pixel width 8\u00b5m, image area 29.18\u00d70.2mm, 14 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"151\"><span style=\"color: #000000;\"><strong>UC-12T2<\/strong><\/span><\/td><td style=\"text-align: center;\" width=\"500\"><span style=\"color: #000000;\">TCD1205 image sensor, spectral range 200-1100nm, non-cooled, 2048 pixels, pixel width 14\u00b5m, image area 28.672\u00d70.2mm,14 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"151\"><span style=\"color: #000000;\"><strong>U2C-14H13496<\/strong><\/span><\/td><td style=\"text-align: center;\" width=\"500\"><span style=\"color: #000000;\">S13496 image sensor, spectral range 200-1000nm, non-cooled, 4096 pixels, pixel size 7 \u00b5m, 14 bit digitization<\/span><\/td><\/tr><tr><td style=\"text-align: center;\" width=\"151\"><span style=\"color: #000000;\"><strong>U2C-14H11639<\/strong><\/span><\/td><td style=\"text-align: center;\" width=\"500\"><span style=\"color: #000000;\">S11639-01 image sensor, spectral range 200-1000nm, non-cooled, 2048 pixels, pixel size 14 \u00b5m, 14 bit digitization<\/span><\/td><\/tr><\/tbody><\/table><p style=\"text-align: center;\"><span style=\"color: #000000;\">\u200b<\/span><\/p><\/div>\n\t\t\t\t\t\t\t\t\t<div class=\"elementor-tab-title elementor-tab-mobile-title\" aria-selected=\"false\" data-tab=\"4\" role=\"tab\" tabindex=\"-1\" aria-controls=\"elementor-tab-content-1024\" aria-expanded=\"false\">OPTICAL BENCH FEATURES<\/div>\n\t\t\t\t\t<div id=\"elementor-tab-content-1024\" class=\"elementor-tab-content elementor-clearfix\" data-tab=\"4\" role=\"tabpanel\" aria-labelledby=\"elementor-tab-title-1024\" tabindex=\"0\" hidden=\"hidden\"><h4 class=\"title-tab title text-left\"><span style=\"color: #000000;\">OPTICAL BENCH FEATURES<\/span><\/h4><p><span style=\"color: #000000;\">The M266 monochromator-spectrograph is built on a modified Czerny-Turner bench, in which the entrance slit and the exit slit (the center of the spectrum) are arranged asymmetrically with respect to the diffraction grating. While developing an optical bench, this arrangement of optical components allows to considerably compensate aberrations inherent to spectral instruments with spherical mirrors, and to obtain the best spectral resolution.<\/span><\/p><p><span style=\"color: #000000;\">In contrast to the broad range of monochromators, whose mechanisms of scanning and changing of diffraction gratings are combined, the M266 uses separate control for scanning and changing of gratings. As a result, an axis of grating rotation is the axis passing through the center of the grating. This design feature, together with the optimisation of linear and angular characteristics of the optical system, has allowed to completely eliminate beam re-reflections on optical elements, to provide extremely low stray light and create a perfect flat field for a multi-element detector.<\/span><\/p><p><span style=\"color: #000000;\">The flat field, in its turn, enables high-quality program sewing of spectra obtained with the multi-element detector by means of several scans.<\/span><\/p><p>\u00a0<\/p><p><span style=\"color: #000000;\">Astigmatism compensation (Imaging option)<\/span><\/p><p><span style=\"color: #000000;\">The astigmatism compensator is a cylindrical mirror which is installed after the entrance slit instead of a flat rotating mirror and provides astigmatism compensation for both output ports (the Imaging version).<\/span><\/p><p><span style=\"color: #000000;\">Astigmatism is common to all spectral instruments; this is a phenomenon when the point on the entrance slit is displayed in the image plane as a vertical segment. The M266 astigmatic segment is 2.4mm in the center of its output flat field, and respectively 2.1mm and 2.8mm at the edges of the field. Astigmatism does not usually impair resolution of the instrument, but, depending on the height of the detector used, can affect the overall sensitivity of the system.<\/span><\/p><p><span style=\"color: #000000;\">Astigmatism correction is imperative in a multichannel spectroscopy, in case you need to adequately transfer the light distribution along the slit, as well as for the use of spectrographs with two-dimensional detectors in the Imaging mode.<\/span><\/p><p><span style=\"color: #000000;\">Introducing the astigmatism compensator in the M266 optical scheme allows correcting astigmatism in the exit slit plane to the value of about 50 micrometers. This fact must be considered when estimating the expected optical resolution of an instrument with a specific grating. Astigmatism compensation also affects the vertical magnification of the spectrograph:<\/span><\/p><table border=\"1\"><thead><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">M266 MAGNIFICATION<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">HORIZONTAL MAGNIFICATION<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">VERTICAL MAGNIFICATION<\/span><\/td><\/tr><\/thead><tbody><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">without astigmatism compensation (Standard mode)<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">1.19<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">1.32<\/span><\/td><\/tr><tr><td style=\"text-align: center;\"><span style=\"color: #000000;\">with astigmatism compensation (Imaging mode)<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">1.19<\/span><\/td><td style=\"text-align: center;\"><span style=\"color: #000000;\">1.55<\/span><\/td><\/tr><\/tbody><\/table><p><span style=\"color: #000000;\"><strong>SPECTRA ACQUIRED WITH THE M266<\/strong><\/span><\/p><p><span style=\"color: #000000;\"><strong>Singlet oxygen spectra*<\/strong><\/span><\/p><p><span style=\"color: #000000;\"><img decoding=\"async\" class=\"aligncenter\" src=\"https:\/\/www.anjun.com.tw\/wp-content\/uploads\/2019\/01\/spectr_1.png\" \/><\/span><\/p><h4><span style=\"color: #000000;\"><em>Emission spectrum of singlet oxygen in the 1268nm band in the supersonic flow. The M266 with the 400 lines\/mm grating and the multi-channel InGaAs detector G9212-512S, entrance slit width 50\u00b5m<\/em><\/span><\/h4><p><span style=\"color: #000000;\"><img decoding=\"async\" class=\"aligncenter\" src=\"https:\/\/www.anjun.com.tw\/wp-content\/uploads\/2019\/01\/spectr_2.png\" \/><\/span><\/p><p><span style=\"color: #000000;\"><em>Emission spectrum of singlet oxygen at the gas generator output. The M266 with the 400 lines\/mm grating and the multi-channel InGaAs detector G9212-512S, entrance slit width 400\u00b5m<\/em><\/span><\/p><h4><span style=\"color: #000000;\"><img decoding=\"async\" class=\"aligncenter\" src=\"https:\/\/www.anjun.com.tw\/wp-content\/uploads\/2019\/01\/spectr_3.png\" \/><\/span><\/h4><p><span style=\"color: #000000;\"><em>Oxygen emission spectrum in the bands 634nm and 703nm, arising from the collision of two singlet-oxygen molecules with their transition to the ground state, one molecule becoming vibrationally excited. The M266 with the 600 lines\/mm grating and multi-channel InGaAs detector G9212-512S, entrance slit width 50 \u00b5m<\/em><\/span><\/p><h4><span style=\"color: #000000;\"><img decoding=\"async\" class=\"aligncenter\" src=\"https:\/\/www.anjun.com.tw\/wp-content\/uploads\/2019\/01\/spectr_4.png\" \/><\/span><\/h4><p><span style=\"color: #000000;\"><em>The peak on the left is the spectrum arising from collision of two singlet-oxygen molecules with their transition to the ground state. The right spectrum in the 763nm band is emission of oxygen in the second electronically excited state<\/em><\/span><\/p><p><span style=\"color: #000000;\">* Courtesy of Lebedev Physical Institute of the Academy of Sciences, Samara Branch, Samara, Russia.<\/span><\/p><p>\u00a0<\/p><p><span style=\"color: #000000;\"><strong>Emission spectra. Quadruplet Fe at 310nm<\/strong><\/span><\/p><h4><span style=\"color: #000000;\"><img decoding=\"async\" class=\"aligncenter\" src=\"https:\/\/www.anjun.com.tw\/wp-content\/uploads\/2019\/01\/M266_fe-quad-1024x749.jpg\" \/><\/span><\/h4><p><span style=\"color: #000000;\"><em>Fe quadruplet, spectral lines 309.9897nm, 309.9971nm, 310.0304nm and 310.0666nm. The spectrum was acquired with spark excitation using the M266 with 1800 lines\/mm grating. The possibility of resolving at least 3 peaks demonstrates high optical quality of the instrument<\/em>\u00a0\u00a0\u00a0<\/span><\/p><h4>\u00a0<\/h4><\/div>\n\t\t\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-b0f1bef elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"b0f1bef\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-e49a9f6\" data-id=\"e49a9f6\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-2e45e8f 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class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-b1817aa elementor-widget elementor-widget-text-editor\" data-id=\"b1817aa\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p style=\"text-align: center;\">SOLARLS\u7684\u6240\u6709\u8cc7\u8a0a\u4f86\u81eaSOLARLS\u7db2\u9801\uff0c\u6240\u6709\u7248\u6b0a\u6b78SOLARLS\uff0c\u7e41\u9ad4\u5b57\u7248\u6b0a\u5c6c\u5b89\u5747\u79d1\u6280\u3002<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>","protected":false},"excerpt":{"rendered":"<p>Model M266 DESCRIPTION SPECIFICATIONS OPTIONS &amp; ACC&hellip;&nbsp;<a href=\"https:\/\/www.anjun.com.tw\/en\/%e9%9b%b7%e5%b0%84\/%e9%9b%b7%e5%b0%84%e9%80%b1%e9%82%8a%e8%a8%ad%e5%82%99%e9%8a%b7%e5%94%ae\/solar-ls%e9%9b%b7%e5%b0%84\/spectral-instruments\/monochromators-spectrographs\/automated-monochromator-spectrograph-2\/\" class=\"\" rel=\"bookmark\">Read More &raquo;<span class=\"screen-reader-text\">AUTOMATED MONOCHROMATOR-SPECTROGRAPH<\/span><\/a><\/p>","protected":false},"author":2,"featured_media":0,"parent":949,"menu_order":16,"comment_status":"closed","ping_status":"closed","template":"","meta":{"neve_meta_sidebar":"","neve_meta_container":"","neve_meta_enable_content_width":"off","neve_meta_content_width":70,"neve_meta_title_alignment":"","neve_meta_author_avatar":"","neve_post_elements_order":"","neve_meta_disable_header":"","neve_meta_disable_footer":"","neve_meta_disable_title":"","footnotes":""},"class_list":["post-1002","page","type-page","status-publish","hentry"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.0 - 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