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Page 5 - Lamp-Pumped

Litron Nano T 135-15 PIV
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Litron Nano T 135-15 PIV
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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
Data Sheet
Litron Nano T 180-15 PIV
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Litron Nano T 180-15 PIV
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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
Data Sheet
Litron Nano L 50-100 PIV
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Litron Nano L 50-100 PIV
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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
Data Sheet
Litron Nano L 100-50 PIV
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Litron Nano L 100-50 PIV
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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
Data Sheet
Litron Nano L 50-50 PIV
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Litron Nano L 50-50 PIV
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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
Data Sheet
Litron Nano L 150-20 PIV
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Litron Nano L 150-20 PIV
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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
Data Sheet
Litron Nano S 65-15 PIV
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Litron Nano S 65-15 PIV
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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
Data Sheet
Litron Nano S 50-20 PIV
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Litron Nano S 50-20 PIV
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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
Data Sheet
Litron Nano S 30-30 PIV
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Litron Nano S 30-30 PIV
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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
Data Sheet
Litron Nano S 30-15 PIV
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Litron Nano S 30-15 PIV
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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
Data Sheet
Litron Bernoulli B-PIV 100-25
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Litron Bernoulli B-PIV 100-25
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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
Data Sheet
Litron Bernoulli B-PIV 145-15
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Litron Bernoulli B-PIV 145-15
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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
Data Sheet
Litron Nano LG 130-50 Laser
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Litron Nano LG 130-50 Laser
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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
...
Data Sheet
Litron Nano LG 200-20 Laser
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Litron Nano LG 200-20 Laser
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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
...
Data Sheet
Litron Nano LG 250-20 Laser
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Litron Nano LG 250-20 Laser
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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
Litron Nano LG 225-10 Laser
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Litron Nano LG 225-10 Laser
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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
Litron Nano LG 300-10 Laser
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Litron Nano LG 300-10 Laser
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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
Litron Nano SG 60-30 Laser
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Litron Nano SG 60-30 Laser
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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
Litron Nano SG 120-20 Laser
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Litron Nano SG 120-20 Laser
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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
Litron Nano SG 150-10 Laser
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Litron Nano SG 150-10 Laser
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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
Litron Nano T 250-20 Laser
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Litron Nano T 250-20 Laser
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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
Litron Nano T 270-20 Laser
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Litron Nano T 270-20 Laser
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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
Litron Nano T 250-10 Laser
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Litron Nano T 250-10 Laser
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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
Litron Nano T 290-10 Laser
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Litron Nano T 290-10 Laser
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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
Litron Nano L 90-100 Laser
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Litron Nano L 90-100 Laser
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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