Litron Nano L 200-15 PIV
Description
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 independent lasers. The range of PIV systems is based around both the ultra-compact Nano series and the larger invar stabilised LPY and LDY series. The overriding factor that sets Litron’s products apart is quality. This is evidenced not only in the design and construction of the product, but also in its performance.
Litron Nano L 200-15 PIV
Specifications |
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|---|---|
| Wavelength: | 532 nm |
| Pulse Energy: | 200 mJ |
| Pulse Energy Stability: | 2 % |
| Pulse Duration: | 9 ns |
| Repetition Rate: | 0-15Hz |
Features
Compact dual head design
Dedicated PIV laser head
Stable resonator design
Telescopic versions for low divergence
Rugged for industrial environments
3rd and 4th harmonics available for LIF and dual colour PIV
Rep. rates to 15Hz
Energies up to 200mJ @ 532nm
Applications
Stable Resonator
Gaussian Optics
Telescopic Resonator
Optical Attenuator
For pricing, technical or any other questions please contact the 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 Litron Nano L 200-15 PIV laser system has an output energy of up to 200mJ at 532nm.
The maximum repetition rate for flashlamp pumped PIV laser systems is up to 200Hz.
Flashlamp pumped PIV laser systems use flashlamps to pump the laser, while diode pumped PIV laser systems use diodes to pump the laser.
Yes, the Litron Nano L 200-15 PIV laser system is rugged and designed for use in industrial environments.
Stable resonator configurations produce a smooth spatial profile that remains homogeneous as it propagates through to the far field, while unstable resonator configurations often have significant structure in the near to intermediate fields, making them unsuitable for forming uniform light sheets.