Nano S 130-10 Laser

Name: Nano S 130-10 Laser
Brand: Litron Lasers
Availability: InStock

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.

Specifications

Wavelength:	532 nm
Pulse Energy:	65 mJ
Pulse Energy Stability:	2 %
Pulse Duration:	6 ns
Repetition Rate:	Not Specified
Optional Wavelengths:	1064nm, 355nm, 266nm, 213nm

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Applications

Spectroscopy
Remote Sensing
Photochemistry
Non-Linear Optics
OPO Pumping
Ablation
ESPI
LIDAR
LIBS
LIF

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Ships from:

United Kingdom

Sold by:

Litron Lasers

On FindLight:

since 2016

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Frequently Asked Questions

What is the difference between the Nano S, Nano L, and Nano T laser heads?

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.

What is the Nano S 130-10 Laser used for?

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.

Can the Nano S be configured with a true TEM00 output?

Yes, the Nano S can be configured with an intra-cavity aperture to give a true TEM00 output.

What is the maximum repetition rate for the Nano L laser head?

The Nano L laser head has a maximum repetition rate of up to 100Hz.

What is the maximum output energy for the Nano T laser head?

The Nano T laser head has a maximum output energy of up to 290mJ.