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Page 6 - Lamp-Pumped

Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 250 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 7 ns
Repetition Rate: 0-20Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 135 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 9 ns
Repetition Rate: 0-15Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 180 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 9 ns
Repetition Rate: 0-15Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 50 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 8 ns
Repetition Rate: 0-100Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 100 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 8 ns
Repetition Rate: 0-50Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 50 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 8 ns
Repetition Rate: 0-50Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 150 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 9 ns
Repetition Rate: 0-20Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 65 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 8 ns
Repetition Rate: 0-15Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 50 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 8 ns
Repetition Rate: 0-20Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head contains two totally ...

Specifications

Wavelength: 532 nm
Pulse Energy: 30 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 8 ns
Repetition Rate: 0-30Hz
Litron offers an extensive range of flashlamp pumped and diode pumped PIV laser systems with output energies of up to 1J per pulse and repetition rates of up to 200Hz for flashlamp systems and up to 20kHz for diode pumped systems. All of the systems are twin head devices, meaning that the PIV laser head ...

Specifications

Wavelength: 532 nm
Pulse Energy: 30 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 8 ns
Repetition Rate: 0-15Hz
The bernoulli™ PIV from Litron is the most advanced ‘plug and play’ PIV laser system available today. It benefits from Litron’s years of experience in this field and the expertise gained from being the World’s leading PIV laser manufacturer.

Specifications

Wavelength: 532 nm
Pulse Energy: 100 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 10 ns
Repetition Rate: 0-25Hz
The bernoulli™ PIV from Litron is the most advanced ‘plug and play’ PIV laser system available today. It benefits from Litron’s years of experience in this field and the expertise gained from being the World’s leading PIV laser manufacturer.

Specifications

Wavelength: 532 nm
Pulse Energy: 145 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 10 ns
Repetition Rate: 0-15Hz
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: 130 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 4 ns
Repetition Rate: 0-50Hz
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: 40 mJ
Pulse Energy Stability: 2 %
Pulse Duration: 4 ns
Repetition Rate: 0-20Hz
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
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
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
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
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