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Page 43 - Solid State Lasers

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 ...

Specifications

Wavelength: 266 nm
Pulse Energy: 30 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 4 ns
Repetition Rate: 0-20Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 213 nm
Pulse Energy: 10 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 4 ns
Repetition Rate: 0-10Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 1064 nm
Pulse Energy: 300 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 4 ns
Repetition Rate: 0-10Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 532 nm
Pulse Energy: 35 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 6 ns
Repetition Rate: 0-30Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 355 nm
Pulse Energy: 15 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 6 ns
Repetition Rate: 0-20Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 266 nm
Pulse Energy: 15 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 4 ns
Repetition Rate: 0-10Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 1064 nm
Pulse Energy: 20 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 7 ns
Repetition Rate: 0-20Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 532 nm
Pulse Energy: 135 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 7 ns
Repetition Rate: 0-20Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 355 nm
Pulse Energy: 45 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 7 ns
Repetition Rate: 0-10Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 266 nm
Pulse Energy: 27 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 7 ns
Repetition Rate: 0-10Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 1064 nm
Pulse Energy: 90 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 7 ns
Repetition Rate: 0-100Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 1064 nm
Pulse Energy: 150 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 7 ns
Repetition Rate: 0-50Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 1064 nm
Pulse Energy: 200 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 6 ns
Repetition Rate: 0-20Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 1064 nm
Pulse Energy: 200 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 6 ns
Repetition Rate: 0-10Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 1064 nm
Pulse Energy: 340 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 7 ns
Repetition Rate: 0-10Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 1064 nm
Pulse Energy: 30 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 6 ns
Repetition Rate: 0-50Hz
...
Data Sheet
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 ...

Specifications

Wavelength: 1064 nm
Pulse Energy: 60 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 6 ns
Repetition Rate: 0-30Hz
...
Data Sheet
The Aurora II-532 Integra range of type II BBO OPOs has been designed with reliability, stability and ease of use in mind. This allows researchers to concentrate on their experiments and industrial systems integrators the peace of mind that their process will be consistent and robust. With a wide choice of integrated ...

Specifications

Total Tuning Range: 670-1064nm
Core Tuning Range: 1065-2300nm
Pulse Energy: 60 mJ
Repetition Rate: 10 Hz
Signal Polarization: Horizontal
...
Data Sheet
The EPEE-30 combines the advantages of a free-space solid state amplifier and fiber laser technology to produce 30W of output power, 200µJ pulse energies, and sub 15ps pulse widths. The fiber seed allows the laser to be more stable, compact, and operationally flexible than traditional solid-state seed lasers. The solid state ...

Specifications

Avg. Power: 30 W
Wavelength: 1064 nm
Repetition Rate: 150-1000kHz
Spatial Mode (M^2): 1.3
Pulse Duration: 0.015 ns
...
Data Sheet
The P302 combines the advantages of an advanced free-space solid state amplifier and fiber laser technology to achieve excellent beam divergence and very narrow pulse widths at high power outputs. The fiber seed allows the laser to be more stable, compact, and operationally flexible than traditional solid state seed lasers. The solid ...

Specifications

Avg. Power: 10 W
Wavelength: 1064 nm
Repetition Rate: 50-500kHz
Spatial Mode (M^2): 1.3
Pulse Duration: 0.015 ns
...
Data Sheet
The MP series UV lasers feature a dual laser diode pumped crystal architecture that produces high power output at the 355 nm wavelength. Advanced resonant cavity design and laser control technology ensure excellent beam quality and narrow pulse widths during high power operation. Special thermal compensation and harmonic generation ...

Specifications

Avg. Power: 7 W
Wavelength: 355 nm
Repetition Rate: 20-100kHz
Spatial Mode (M^2): 1.3
Pulse Duration: 25 ns
...
Data Sheet
The Delphi ultraviolet series lasers take advantage of an advanced resonant cavity design and cutting-edge laser control system to deliver superior beam divergence and narrow pulse widths at high-power work settings. The gain medium is composed of Nd:YVO4.

Specifications

Avg. Power: 10 W
Wavelength: 355 nm
Repetition Rate: 40-100kHz
Spatial Mode (M^2): 1.3
Pulse Duration: 20 ns
...
Data Sheet
The PS100-G combines the advantages of a free-space solid state amplifier and fiber laser technology to produce greater than 2W of output power at a pulse repetition rate of 500kHz, sub 15ps pulse widths, and beam quality of M2

Specifications

Avg. Power: 2 W
Wavelength: 1064 nm
Repetition Rate: 50-1000kHz
Spatial Mode (M^2): 1.3
Pulse Duration: 0.015 ns
...
Data Sheet
The LP series UV Laser uses an advanced resonant cavity and laser control system to achieve better beam divergence and narrower pulse width in high power work settings.

Specifications

Avg. Power: 3 W
Wavelength: 355 nm
Repetition Rate: 20-100kHz
Spatial Mode (M^2): 1.3
Pulse Duration: 20 ns
...
The LP104 Diode Pumped UV Laser uses an advanced resonant cavity and laser control system to achieve better beam divergence and narrower pulse width in high power work settings.

Specifications

Avg. Power: 3 W
Wavelength: 355 nm
Repetition Rate: 20-200kHz
Spatial Mode (M^2): 1.3
Pulse Duration: 20 ns
...