On this page, we have a list of all of the 33Hz repetition (rep) rate lasers offered by RPMC. If you don’t see a laser with the parameters needed, most of our lasers can be modified for your needs.
For pulsed lasers, unlike continuous-wave (CW) lasers, the output cannot be specified by their output power alone. This is because the output power of a pulsed laser is determined by three different parameters; the laser’s pulse width, pulse energy, and pulse repetition rate.
If you need help selecting the best laser for your application, or defining the laser requirements for a specific application, please contact our product manager for assistance.
The Q-TUNE-G series is a highly advanced air-cooled, tunable wavelength laser with seamless OPO integration. It offers hands-free, automated tuning from 680 to 2100 nm, delivering up to 12 mJ pulse energy in the near-IR range. With a <10 cm-¹ linewidth and up to 100 Hz pulse repetition rate, it’s ideal for photoacoustic imaging, non-linear spectroscopy, and more. The user-friendly web interface and microprocessor control ensure ease of use, while the water-free, air-cooled pump laser design optimizes performance. The Q-TUNE-G series sets a new standard in precision and efficiency for researchers across disciplines.
The Q-TUNE series is a highly efficient, tunable wavelength laser designed for researchers working with temporally resolved spectroscopy, metrology, photo-acoustic imaging, and remote sensing applications. This laser uses an optical parametric oscillator (OPO) to produce a tunable wavelength range of 410-2300 nm with a linewidth narrower than 6 cm-1, which can be extended to 210-410 nm with an optional second harmonic generator. With a pulse duration shorter than 5ns and an upper repetition rate of 100Hz, the Q-TUNE series provides a perfect coherent light source for precise scientific measurements.
The Q-SHIFT series of Q-switched DPSS lasers is designed for researchers and application specialists working in micromachining, dermatology, LIDAR, time-resolved laser spectroscopy, and LIBS applications. With its built-in nonlinear wavelength conversion stage, this series allows the production of unconventional fundamental DPSS wavelengths, including 1163, 1177, 1300, 1317, 1551 and 1571 nm options, making it an ideal choice for those seeking wavelengths that are not accessible with conventional solid-state laser sources. With the optional harmonics generator, it is possible to generate up to the 4th harmonic for each fundamental wavelength, providing even more versatility.