Litron Nano S 30-50 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 S 30-50 Laser
Specifications |
|
|---|---|
| Wavelength: | 1064 nm |
| Pulse Energy: | 30 mJ |
| Pulse Energy Stability: | 2 % |
| Pulse Duration: | 6 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
- No registration required
- No markups, no fees
- Direct contact with supplier
Contact Supplier
How to order?
-
Ships from:
United Kingdom
-
Sold by:
-
On FindLight:
since 2016
Frequently Asked Questions
The applications of the Litron Nano S 30-50 Laser include spectroscopy, remote sensing, photochemistry, non-linear optics, OPO pumping, ablation, PIV, ESP, LIDAR, LIBS, and LIF.
The maximum repetition rate of the Nano T model of the Litron Nano S 30-50 Laser ranges from 10 to 50 Hz, depending on the specific model.
The maximum output energy of the Nano S model of the Litron Nano S 30-50 Laser ranges from 30 to 340 mJ, depending on the specific model.
The pointing stability of the Nano T model of the Litron Nano S 30-50 Laser is less than 70 µrad.
The output of the Litron Nano S 30-50 Laser is multimode.