Litron Nano LG 130-50 Laser
Description
The Nano range allows a great deal of flexibility both in scientific and industrial applications. The output of these systems is multimode, however the telescopic resonators offer high energy beams with low divergences - comparable to those from unstable Gaussian coupled resonators but with a more uniform spatial profile, and a smoother temporal profile.
Litron Nano LG 130-50 Laser
Specifications |
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|---|---|
| Wavelength: | 1064 nm |
| Pulse Energy: | 130 mJ |
| Pulse Energy Stability: | 2 % |
| Pulse Duration: | 4 ns |
| Repetition Rate: | 0-50Hz |
| Optional Wavelengths: | 532nm, 355nm, 266nm, 213nm |
Applications
Remote Sensing
Photochemistry
Non-Linear Optics
OPO Pumping
Ablation
PIV
ESPI
LIDAR
LIBS
LIF
For pricing, technical or any other questions please contact the supplier
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How to order?
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Ships from:
United Kingdom
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Sold by:
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On FindLight:
since 2016
Frequently Asked Questions
The applications of the Litron Nano LG 130-50 Laser include spectroscopy, remote sensing, photochemistry, non-linear optics, OPO pumping, ablation, PIV, ESPI, LIDAR, LIBS, and LIF.
The maximum repetition rate of the Nano T model ranges from 10 Hz to 50 Hz depending on the specific model.
The ambient temperature range for the Nano S and Nano L models is 5-35 ˚C.
The Nano range offers stable and stable telescopic resonators.
The output of the Litron Nano LG 130-50 Laser is multimode.