Nano S 130-10 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.
Nano S 130-10 Laser
Specifications |
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|---|---|
| Wavelength: | 532 nm |
| Pulse Energy: | 65 mJ |
| Pulse Energy Stability: | 2 % |
| Pulse Duration: | 6 ns |
| Repetition Rate: | 0-10Hz |
| Optional Wavelengths: | 1064nm, 355nm, 266nm, 213nm |
Applications
Spectroscopy
Remote Sensing
Photochemistry
Non-Linear Optics
OPO Pumping
Ablation
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
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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 Nano S, Nano L, and Nano T laser heads are all fundamentally the same construction, but differ in size and output energies. The Nano S is the smallest with energies up to 150mJ per pulse, the Nano L has a footprint of only 380mm x 96mm with output energies up to 340mJ, and the Nano T has a footprint of 520mm x 96mm with output energies up to 290mJ.
The Nano S 130-10 Laser can be used for a variety of applications including spectroscopy, remote sensing, photochemistry, non-linear optics, OPO pumping, ablation, ESPIL, LIDAR, and LIBS.
Yes, the Nano S can be configured with an intra-cavity aperture to give a true TEM00 output.
The Nano L laser head has a maximum repetition rate of up to 100Hz.
The Nano T laser head has a maximum output energy of up to 290mJ.