{"id":230,"date":"2021-09-04T16:13:37","date_gmt":"2021-09-04T16:13:37","guid":{"rendered":"https:\/\/beamq.com\/laser\/?p=230"},"modified":"2022-01-13T04:01:13","modified_gmt":"2022-01-13T04:01:13","slug":"266nm-ultraviolet-solid-state-dpss-pulsed-laser","status":"publish","type":"post","link":"https:\/\/beamq.com\/laser\/266nm-ultraviolet-solid-state-dpss-pulsed-laser\/","title":{"rendered":"266nm UltraViolet Solid State DPSS Pulsed Laser"},"content":{"rendered":"\n<p><\/p>\n\n\n\n<p>All kinds of 266nm DPSS Laser , Other <a href=\"https:\/\/www.beamq.com\/dpss-laser-solid-266nm400nm-uv-c-66_103.html\">DPSS Lasers from 266nm-400nm UV<\/a> .<\/p>\n\n\n\n<p><\/p>\n\n\n\n<p><a href=\"https:\/\/www.rpmclasers.com\/wavelength\/266nm-lasers\/\">266nm from rpmclasers<\/a><\/p>\n\n\n\n<p>266nm Lasers, specifically Diode-Pumped Solid-State (DPSS) Lasers, utilize the fourth harmonic of Nd:YAG laser material at 1064nm. Given a particular laser, with a particular fundamental wavelength, fourth harmonic generation is less efficient and cannot achieve the same energy levels compared to its lower-order harmonic counterparts.<\/p>\n\n\n\n<p>These high power, nanosecond 266nm lasers are available with either free-space or fiber-coupled output and a variety of pulse energies depending on the applications needs. Typical applications for these UV Lasers include Optogenetics, Laser Induced Breakdown Spectroscopy, Time-of-Flight Spectroscopy, Photoluminescence, and more.<\/p>\n\n\n\n<p>Contact us for a quote, for technical support, or help in selecting the best laser.<\/p>\n\n\n\n<p><\/p>\n\n\n\n<p><a href=\"http:\/\/www.roithner-laser.com\/laser_systems_266.html\">DIODE PUMPED SOLID STATE LASER SYSTEMS &#8211; 266 nm from Roithner Lasertechnik GmbH<\/a><\/p>\n\n\n\n<p>Passively Q-switched ultraviolet laser at 266 nm<\/p>\n\n\n\n<p>Operation Mode: Q-switchedSeperate laser head, cooled by TECPower supply included, fixed output power, 90-264 VAC<\/p>\n\n\n\n<p><a href=\"https:\/\/www.beamq.com\/266nm-ultraviolet-solid-state-dpss-pulsed-laser-p-260.html\">266nm UltraViolet Solid State DPSS Pulsed Laser<\/a><\/p>\n\n\n\n<p>Wavelength (nm):266\u00b11<br>Repetition Rate:1-100Hz<br>Single pulse energy (mJ): 2<br>Energy Stability2(RMS): &lt;4%<br>Pulse Width: &lt; 10ns<br>Divergence: 2 mrad<br>PointingStability: 50 urad<br>Beam parameters : 3mm<br>Output average power (mW): 1~20<br>Transverse mode: Near TEM00<br>Operating mode: Frequency conversion of Q-switched pulsed laser<br>Pulse duration (ns): ~7<br>FWHM:0.2nm<br>Rep. rate (kHz):<\/p>\n\n\n\n<p>Controllable Fixed rep. rate, such as 1k, 2k, 3k, 4k, 5kHz, with stable laser pulses emitting (stable pulse energy, peak, duration and period);<br>Different rep. rate in th Rep. rate (kHz) the range of 1kHz-5kHz can be obtained by input an external TTL signal;<br>Uncontrollable: Undefined rep. rate among 5k-7kHz and unstable laser pulse emitting. Suitable\u00c2 for the applications only needing high peak power pulses;<\/p>\n\n\n\n<p>Average power (mW): Average power (mW) = Single pulse energy (\u03bcJ) * Rep. rate (kHz)<\/p>\n\n\n\n<p>M2 factor : &lt;1. 5 Polarization ratio : &gt;100:1<br>Warm-up time (minutes): &lt;10<br>Expected lifetime (hours): 10000<br>Warranty period: 1 year<\/p>\n\n\n\n<p>Because of the Walk-off effect of Nonlinear crystals, the beam quality of UV laser is not so good as that of 1064\/532nm laser.<\/p>\n\n\n\n<p>Applications:<br>Raman measurements<\/p>\n\n\n\n<p>266 nm Beam Splitting Principle as following:<\/p>\n\n\n\n<p>It can be Passively Q-switched and Actively Q-switched<\/p>\n","protected":false},"excerpt":{"rendered":"<p>All kinds of 266nm DPSS Laser , Other DPSS Lasers from 266nm-400nm UV . 266nm from rpmclasers 266nm Lasers, specifically Diode-Pumped Solid-State (DPSS) Lasers, utilize the fourth harmonic of Nd:YAG laser material at 1064nm. Given a particular laser, with a particular fundamental wavelength, fourth harmonic generation is less efficient and cannot achieve the same energy [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":[],"categories":[57],"tags":[56],"_links":{"self":[{"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/posts\/230"}],"collection":[{"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/comments?post=230"}],"version-history":[{"count":4,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/posts\/230\/revisions"}],"predecessor-version":[{"id":607,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/posts\/230\/revisions\/607"}],"wp:attachment":[{"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/media?parent=230"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/categories?post=230"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/beamq.com\/laser\/wp-json\/wp\/v2\/tags?post=230"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}