Ekspla ANL series electro-optically Q-switched nanosecond Nd:YAG amplifier systems deliver high energy pulses at high repetition rates.

A diode-pumped Q-switched nanosecond laser, based on industry-tested technology is used as a master oscillator of the system. It produces high-intensity, high-brightness pulses and is well suited for further amplification in linear amplifiers for high-energy Super-Gaussian output pulses. Employing electro-optical cavity dumping, the master oscillator can produce pulses which are as short as several ns with uniform beam profile and low divergence.

Alternatively customers own seed source can be implemented as master oscillator and amplified to required energy level for further amplification in main power amplifiers.

Power amplifiers are a chain of low-maintenance diode-pumped single and double pass amplifiers where pulses are amplified up to the required energy. During amplification, spatial beam shaping is employed in order to get a Super-Gaussian beam shape at the output.

Angle-tuned non-linear crystals harmonic generators mounted in temperature stabilized heaters are used for second and third harmonic generation. Harmonic separation system is designed to ensure high spectral purity of radiation and direct it to the output ports.

System control is available through control pad, USB and LAN interfaces (RS232 as optional). The system can be controlled from personal computer with supplied software for Windows operating system.

To tailor the laser for specific applications or requirements, various customization possibilities are available such as industrial grade, portable laser housing with integrated power supplies and cooling units; customer’s seed integration; multi-channel outputs; burst amplification and various other.

Angle-tuned non-linear crystals harmonic generators mounted in temperature stabilized heaters are used for second and third harmonic generation. Harmonic separation system is designed to ensure high spectral purity of radiation and direct it to the output ports.

System control is available through control pad, USB and LAN interfaces (RS232 as optional). The system can be controlled from personal computer with supplied software for Windows operating system.

To tailor the laser for specific applications or requirements, various customization possibilities are available such as industrial grade, portable laser housing with integrated power supplies and cooling units; customer’s seed integration; multi-channel outputs; burst amplification and various other.

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  • Up to 3.7 J at 1064 nm output pulse energy
  • Up to 1 kHz repetition rate
  • Multi-channel version 2 J per channel at 1064 nm
  • Pulse durations from 2 ns to 500 ns
  • Burst version available

FEATURES

  • Up to 3.7 J at 1064 nm output pulse energy
  • Up to 1 kHz repetition rate
  • Multi-channel version 2 J per channel at 1064 nm
  • Pulse durations from 2 ns to 500 ns
  • Spatial Super-Gaussian beam profile
  • Low maintenance cost and long diode lifetime
  • Variable pulse duration and temporal pulse shape control (AWG) option available
  • Various customization possibilities to tailor for specific application
  • High efficiency diode pumping chambers
  • Small laser head footprint and OEM integration upon request
  • Internal system diagnostics
  • Thermally induced birefringence compensation for high pulse repetition rates
  • Integrated vacuum system for image translation for smooth Super-Gaussian beam profile
  • Burst version available
  • Optional thermally stabilized second and third harmonics generators
  • Optional industrial grade, portable laser housing with integrated power supplies and cooling units

APPLICATIONS

  • Thomson Scattering
  • Multi-stage OPCPA pumping
  • Non-linear optics
  • Ti:S pumping

 

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