{"id":12298,"date":"2026-07-17T18:20:53","date_gmt":"2026-07-17T16:20:53","guid":{"rendered":"https:\/\/soliton-gmbh.de\/?post_type=product&#038;p=12298"},"modified":"2026-07-17T18:27:26","modified_gmt":"2026-07-17T16:27:26","slug":"vlite-hi-532-serie-time-resolved-piv","status":"publish","type":"product","link":"https:\/\/soliton-gmbh.de\/en\/produkt\/vlite-hi-532-serie-time-resolved-piv\/","title":{"rendered":"vLite-Hi-532 \u2013 Time-Resolved PIV"},"content":{"rendered":"<p>The <strong data-start=\"483\" data-end=\"505\">vLite-Hi-532 Series<\/strong> from <strong data-start=\"510\" data-end=\"532\">Beamtech Optronics<\/strong> is a family of high-frequency dual-pulse DPSS lasers for demanding <strong data-start=\"605\" data-end=\"641\">Particle Image Velocimetry (PIV)<\/strong>-Applications. The systems are based on a continuously diode-pumped Nd:YAG laser with acousto-optic Q-switching technology and efficient frequency doubling to generate green laser pulses at <strong data-start=\"843\" data-end=\"853\">532nm<\/strong>. You achieve repetition rates of <strong data-start=\"890\" data-end=\"906\">1 to 30 kHz<\/strong>, pulse energies up to <strong data-start=\"925\" data-end=\"945\">12 mJ at 10 kHz<\/strong> as well as an average output power of up to <strong data-start=\"1003\" data-end=\"1012\">120 W<\/strong>.<\/p>\n<p data-start=\"1934\" data-end=\"2304\">The vLite-Hi-532 series utilizes a continuous diode-pumped Nd:YAG laser with acousto-optic Q-switching technology and efficient frequency doubling to generate high-frequency green laser pulses at 532 nm. The system is specifically designed for applications that combine high repetition rates with stable pulse energy.<\/p>\n<p data-start=\"2306\" data-end=\"2719\">With a continuously adjustable repetition rate of <strong data-start=\"2365\" data-end=\"2381\">1 to 30 kHz<\/strong> The series is particularly suitable for modern high-speed PIV systems. Compared to the vLite-Hi-527 series, it offers significantly higher repetition rates, making it especially suitable for time-resolved flow analyses and as a pump source for high-frequency Ti:Sapphire amplifiers.<\/p>\n<p data-start=\"2721\" data-end=\"2989\">The robust industrial design with standardized electrical interfaces simplifies integration into existing measurement and OEM systems. At the same time, the design allows for reliable 24\/7 continuous operation.<\/p>\n<h2 class=\"PDq2pG_selectionAnchorContainer\" data-section-id=\"jiq223\" data-start=\"2996\" data-end=\"3017\">Available Models<\/h2>\n<p data-start=\"3019\" data-end=\"3085\">The <strong data-start=\"3023\" data-end=\"3045\">vLite-Hi-532 Series<\/strong> is available in three performance levels:<\/p>\n<h3 data-section-id=\"u69v9w\" data-start=\"3087\" data-end=\"3106\">vLite-Hi-532-80<\/h3>\n<ul data-start=\"3108\" data-end=\"3206\">\n<li data-section-id=\"yrzu09\" data-start=\"3108\" data-end=\"3145\">Pulse energy <strong data-start=\"3122\" data-end=\"3145\">2 x 8 mJ at 10 kHz<\/strong><\/li>\n<li data-section-id=\"1wgoojc\" data-start=\"3146\" data-end=\"3206\">Average output power <strong data-start=\"3183\" data-end=\"3206\">2 x 80 W at 10 kHz<\/strong><\/li>\n<\/ul>\n<h3 data-section-id=\"1bh5m5\" data-start=\"3208\" data-end=\"3228\">vLite-Hi-532-100<\/h3>\n<ul data-start=\"3230\" data-end=\"3330\">\n<li data-section-id=\"15agtf4\" data-start=\"3230\" data-end=\"3268\">Pulse energy <strong data-start=\"3244\" data-end=\"3268\">2 x 10 mJ at 10 kHz<\/strong><\/li>\n<li data-section-id=\"fwt8jl\" data-start=\"3269\" data-end=\"3330\">Average output power <strong data-start=\"3306\" data-end=\"3330\">2 x 100 W at 10 kHz<\/strong><\/li>\n<\/ul>\n<h3 data-section-id=\"1bh5nz\" data-start=\"3332\" data-end=\"3352\">vLite-Hi-532-120<\/h3>\n<ul data-start=\"3354\" data-end=\"3454\">\n<li data-section-id=\"1dij2b6\" data-start=\"3354\" data-end=\"3392\">Pulse energy <strong data-start=\"3368\" data-end=\"3392\">2 x 12 mJ at 10 kHz<\/strong><\/li>\n<li data-section-id=\"2nns3n\" data-start=\"3393\" data-end=\"3454\">Average output power <strong data-start=\"3430\" data-end=\"3454\">2 x 120 W at 10 kHz<\/strong><\/li>\n<\/ul>\n<p data-start=\"3456\" data-end=\"3756\">All models operate at a wavelength of <strong data-start=\"3504\" data-end=\"3514\">532nm<\/strong>, feature an adjustable repetition rate of <strong data-start=\"3568\" data-end=\"3584\">1 to 30 kHz<\/strong>, an energy stability of <strong data-start=\"3613\" data-end=\"3626\">&lt; 1 % RMS<\/strong> as well as a dual-channel pulse output for demanding high-speed PIV applications.<\/p>\n<h2 data-section-id=\"1s904nn\" data-start=\"3763\" data-end=\"3797\">Advantages of the vLite-Hi-532 Series<\/h2>\n<ul data-start=\"3799\" data-end=\"4094\">\n<li data-section-id=\"14ypo9i\" data-start=\"3799\" data-end=\"3832\">Repetition rates up to <strong data-start=\"3822\" data-end=\"3832\">30kHz<\/strong><\/li>\n<li data-section-id=\"1jxizmw\" data-start=\"3833\" data-end=\"3883\">Average output power to <strong data-start=\"3874\" data-end=\"3883\">120 W<\/strong><\/li>\n<li data-section-id=\"1lca4jk\" data-start=\"3884\" data-end=\"3908\">Pulse duration &lt; <strong data-start=\"3898\" data-end=\"3908\">150 ns<\/strong><\/li>\n<li data-section-id=\"efjavt\" data-start=\"3909\" data-end=\"3933\">High energy stability<\/li>\n<li data-section-id=\"4vgwq7\" data-start=\"3934\" data-end=\"3958\">Dual-channel pulse output<\/li>\n<li data-section-id=\"1dov1of\" data-start=\"3959\" data-end=\"3980\">Continuous operation (24\/7)<\/li>\n<li data-section-id=\"148ci8h\" data-start=\"3981\" data-end=\"4008\">Robust industrial housing<\/li>\n<li data-section-id=\"1k5dsev\" data-start=\"4009\" data-end=\"4035\">Simple OEM Integration<\/li>\n<li data-section-id=\"1b20s8f\" data-start=\"4036\" data-end=\"4094\">Ideal for high-speed PIV and Ti:Sapphire systems<\/li>\n<\/ul>\n<h2 class=\"PDq2pG_selectionAnchorContainer\" data-section-id=\"ppc6sv\" data-start=\"3387\" data-end=\"3400\">Manufacturer<\/h2>\n<p data-start=\"3402\" data-end=\"3665\"><strong data-start=\"3402\" data-end=\"3424\">Beamtech Optronics<\/strong> develops laser sources for industrial, scientific, and fluid mechanics applications. The portfolio includes PIV lasers, DPSS lasers, Nd:YAG lasers, as well as custom laser systems for research, metrology, and OEM integration.<\/p>","protected":false},"excerpt":{"rendered":"<p><a href=\"https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2022\/11\/Zeichenflaeche-1@3x.png\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-9731\" src=\"https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2022\/11\/Zeichenflaeche-1@3x.png\" alt=\"\" width=\"202\" height=\"36\" srcset=\"https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2022\/11\/Zeichenflaeche-1@3x.png 1011w, https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2022\/11\/Zeichenflaeche-1@3x-300x53.png 300w, https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2022\/11\/Zeichenflaeche-1@3x-768x137.png 768w, https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2022\/11\/Zeichenflaeche-1@3x-18x3.png 18w, https:\/\/soliton-gmbh.de\/wp-content\/uploads\/2022\/11\/Zeichenflaeche-1@3x-600x107.png 600w\" sizes=\"auto, (max-width: 202px) 100vw, 202px\" \/><\/a><\/p>\n<ul>\n<li data-section-id=\"owprr1\" data-start=\"1162\" data-end=\"1198\">High-frequency dual-pulse DPSS lasers<\/li>\n<li data-section-id=\"1lgeamq\" data-start=\"1199\" data-end=\"1244\">Specifically for <strong data-start=\"1214\" data-end=\"1244\">Time-Resolved PIV<\/strong><\/li>\n<li data-section-id=\"c64xgm\" data-start=\"1245\" data-end=\"1265\">Wavelength 532 nm<\/li>\n<li data-section-id=\"1yicbim\" data-start=\"1266\" data-end=\"1333\">Continuous adjustable repetition rate from <strong data-start=\"1315\" data-end=\"1333\">1 to 30 kHz<\/strong><\/li>\n<li data-section-id=\"p7435j\" data-start=\"1334\" data-end=\"1372\">Pulse energy up to <strong data-start=\"1353\" data-end=\"1372\">120W at 10 kHz<\/strong><\/li>\n<li data-section-id=\"ah9xey\" data-start=\"1373\" data-end=\"1400\">Pulse durations up to <strong data-start=\"1390\" data-end=\"1400\">150 ns<\/strong><\/li>\n<\/ul>","protected":false},"featured_media":12020,"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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