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The neoMOS laser series combines the reliability and low maintenance of state of the art ultra-short pulsed oscillators with a solid-state amplifier. The ultra-compact laser head has the smallest footprint currently available and enables easy system integration. High stability and long lifetime are provided by design for 24/7 ...
  • Center Wavelength: 1030 nm
  • Repetition Rate: 0 - 20000 kHz
  • Pulse Energy: 0,04 mJ
  • Energy Stability (RMS): <1 %
  • Pulse Duration: 600 fs
  • ...
Data Sheet
The venteon pre-amp modules have been developed for the amplification of low energy pulses (~10 pJ) to significant higher power levels. Designed for amplifying the narrowband 1030 nm output of the venteon dual laser system, the alignment-free preamplifier modules can also be used as an independent amplification module for other laser ...
  • Center Wavelength: 1030 nm
  • Repetition Rate: 300 - 80000 kHz
  • Pulse Energy: 0.0000005 mJ
  • Energy Stability (RMS): -- %
  • Pulse Duration: 10000 fs
  • ...
Data Sheet
The venteon pre-amp modules have been developed for the amplification of low energy pulses (~10 pJ) to significant higher power levels. Designed for amplifying the narrowband 1030 nm output of the venteon dual laser system, the alignment-free preamplifier modules can also be used as an independent amplification module for other laser ...
  • Center Wavelength: 1030 nm
  • Repetition Rate: Determined by seed oscillator - kHz
  • Pulse Energy: 0.000001 mJ
  • Energy Stability (RMS): -- %
  • Pulse Duration: 10000 fs
  • ...
Data Sheet
A powerful industrial laser offering up to 30 W output power at 1030 nm at 1 MHz and above 160 µJ at 100 kHz. Pulses are shorter than 800 fs.
  • Center Wavelength: 1030 nm
  • Repetition Rate: 100 - 1000 kHz
  • Pulse Energy: 0.160 mJ
  • Energy Stability (RMS): 2 %
  • Pulse Duration: 800 fs
  • ...
Data Sheet
The neoMOS picosecond laser series combines the reliability and low maintenance of a state of the art picosecond laser oscillator with a solid-state amplifier. The new developed laser system further expands the neoMOS pulse duration range into the area of less than 2 ps. The CPA free technology allows for bandwidth limited pulses on ...
  • Center Wavelength: 1064 nm
  • Repetition Rate: 50 - 30000 kHz
  • Pulse Energy: 0.03 mJ
  • Energy Stability (RMS): 1 %
  • Pulse Duration: 2000 fs
  • ...
Data Sheet
The neoMOS picosecond laser series combines the reliability and low maintenance of a state of the art picosecond laser diode with a solid-state amplifier. Customized combinations with different output powers and flexible repetition rates are integrated into a ultra-compact laser head enabling easy system integration. High stability ...
  • Center Wavelength: 1064 nm
  • Repetition Rate: 0 - 50000 kHz
  • Pulse Energy: 0.15 mJ
  • Energy Stability (RMS): 1 %
  • Pulse Duration: 70000 fs
  • ...
Data Sheet
The neoMOS picosecond laser series combines the reliability and low maintenance of state of the art picosecond oscillators with a solid-state amplifier. The ultra-compact laser head has the smallest footprint currently available enabling easy system integration. High stability and long lifetime are provided by design for 24/7 ...
  • Center Wavelength: 1064 nm
  • Repetition Rate: 50 - 40000 kHz
  • Pulse Energy: 0.15 mJ
  • Energy Stability (RMS): 1 %
  • Pulse Duration: 10000 fs
  • ...
Data Sheet
The venteon OPCPA provides a unique combination of a few-cycle pulse duration with a pulse energy in the µJ-regime at a high repetition rate. The excellent output stability, and the ability for a CEP-stabilised output, makes this amplifier the ideal source for nonlinear spectroscopy, high harmonic generation and applications in ...
  • Center Wavelength: ... nm
  • Repetition Rate: 200 - 1000 kHz
  • Pulse Energy: 5µJ mJ
  • Energy Stability (RMS): 1 %
  • Pulse Duration: 8fs fs
  • ...
Data Sheet
SL200 Series SBS Compressed Nd:YAG lasers by EKSPLA.SL 200 series lasers are excellent solution for applications, where high energy picosecond pulses are needed. Not like conventional mode-locked lasers that typically uses saturable nonlinear absorption or Kerr lensing to produce ultrafast pulses, the SL200 series lasers employ ...
  • Center Wavelength: 1064 nm
  • Repetition Rate: 0.01 - 0.05 kHz
  • Pulse Energy: 250 mJ
  • Energy Stability (RMS): 3 %
  • Pulse Duration: 100000 fs
  • ...
Data Sheet
APL2200 Series hihg rep rate and high energy amplifiers by EKSPLA. APL2200 series amplifiers are designed to produce up to 60 mJ picosecond pulses at kilohertz pulse repetition rate. Short pulse duration, excellent pulse-to-pulse stability, superior beam quality makes APL2200 series diode pumped picosecond amplifiers well suited for ...
  • Center Wavelength: 1064 nm
  • Repetition Rate: 1 - 1 kHz
  • Pulse Energy: 60 mJ
  • Energy Stability (RMS): 1 %
  • Pulse Duration: 9000 fs
  • ...
Data Sheet
SL Series high energy Nd:YAG lasers by EKSPLA. SL 300 series lasers are an excellent solution for applications that require high energy picosecond pulses. Pulse compression during backward-stimulated Brillouin scattering (SBS), used in EkSPLa SL300 series lasers, is a simple and cost-efficient way to generate picosecond pulses, with ...
  • Center Wavelength: 1064 nm
  • Repetition Rate: 0.005 - 0.05 kHz
  • Pulse Energy: 500 mJ
  • Energy Stability (RMS): 4 %
  • Pulse Duration: 150 fs
  • ...
Data Sheet
PL3140 Series Nd:YLF high energy mode-locked lasers by EKSPLA. Nd:YLF mode-locked PL3143 series picosecond lasers produces high energy pulses with as short as 10 ps pulse duration.
  • Center Wavelength: 1053 nm
  • Repetition Rate: 0.005 - 0.01 kHz
  • Pulse Energy: 80 mJ
  • Energy Stability (RMS): 1.5 %
  • Pulse Duration: 10000 fs
  • ...
Data Sheet
PL11M Series high pulse rep rate mode-locked lasers by EKSPLA. PL11M series picosecond mode‑locked diode pumped laser offers 1 W output power at 1064 nm. It features high 1 MHz repetition rate, short 10 ps pulse duration andexcellent beam quality (M² < 1.5).
  • Center Wavelength: 1064 nm
  • Repetition Rate: 100 - 1000 kHz
  • Pulse Energy: 0.001 mJ
  • Energy Stability (RMS): 2 %
  • Pulse Duration: 10000 fs
  • ...
Data Sheet
PL2230 Series high energy DPSS Mode-Locked Nd:YAG lasers by EKSPLA. EKSPLA is proud to introduce the first commercial fully diode pumped high pulse energy mode-locked laser, producing 28 ps pulses with up to 18 mJ pulse energy at a 100 Hz or up to 40 mJ at at 50 Hz pulse repetition rate.
  • Center Wavelength: 1064 nm
  • Repetition Rate: 0.05 - 0.1 kHz
  • Pulse Energy: 40 mJ
  • Energy Stability (RMS): 0.5 %
  • Pulse Duration: 28000 fs
  • ...
Data Sheet
Picosecond diode pumped mode-locked Nd:YAG laser by EKSPLA. PL2210 series lasers are diode-pumped,air-cooled, mode-locked Nd:YaG lasers produce picosecond pulses at a kilohertz pulse repetition rate. Short pulse duration, excellent pulse-to-pulse stability, superior beamquality makes PL2210 series diode pumped picosecond lasers well ...
  • Center Wavelength: 1064 nm
  • Repetition Rate: 1 - 2 kHz
  • Pulse Energy: 2.5 mJ
  • Energy Stability (RMS): 0.5 %
  • Pulse Duration: 25000 fs
  • ...
Data Sheet
CARBIDE femtosecond laser system by Light Conversion. Pico- and femtosecond lasers are now at the cutting edge of material micro processing in fields ranging from optoelectronics devices to eye surgery. advantage of the ultrafast lasers lies in highly nonlinear interaction of short and intense light pulses with matter when ablation ...
  • Center Wavelength: 1028 nm
  • Repetition Rate: 50 - 1000 kHz
  • Pulse Energy: 0.1 mJ
  • Energy Stability (RMS): 0.28 %
  • Pulse Duration: 290 fs
  • ...
Data Sheet

Did You know?

Advanced ultrafast amplifiers combine high power, excellent beam quality, and high repetition rates. Enormously high optical intensities, exceeding 10^16 W/cm^2, can be achieved by focusing such intense pulses in some medium. There are two typical amplification schemes, one using the Chirped Pulse Amplification (CPA) technique and another based on multi-pass pulse amplification through the amplification medium. Ultrafast amplifiers find applications where intense pulses for highly nonlinear processes, such as high harmonic generation, are required or for the acceleration of particles to high energies. They may be used in laser-induced nuclear fusion or for micromachining.