FemtoLux

Industrial Femtosecond Lasers

FemtoLux is designed from the get-go for maximum reliability, seamless integration and non-stop 24/7/365 zero maintenance operation with innovative ”dry” cooling. Wide range of options enable to tailor this ultrafast laser for desired material processing tasks.

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Features

  • At 1030 nm
    50 W typical max output power
    > 300 µJ typical max output energy
  • At 515 nm
    20 W typical max output power
    > 50 µJ typical max output energy
  • At 343 nm
    10 W typical max output power
    > 25 µJ typical max output energy
  • Up to 1 mJ for FemtoLux HE
  • Up to 2 mJ in a burst mode
  • < 400 fs – 1 ps
  • Pulse duration extension up to 1 ns
  • Single shot – up to 4 MHz (AOM controlled)
  • MHz, GHz, MHz+GHz burst modes
  • Pulse-on-demand (PoD), with jitter as low as 20 ns (peak-to-peak)
  • < 0.5% RMS power long term stability over 100 hours
  • M² < 1.2
  • Beam ellipticity > 0.85
  • Zero maintenance
  • Dry cooling (no water used)
  • PSU and cooling unit integrated into single 4U rack housing
  • Easy and quick installation
  • Compatible with galvo and Polygon scanners as well as PSO controllers

A reliable & versatile tool for micromachining

Designed from the get-go for maximum reliability, seamless integration and non-stop 24/7/365 zero maintenance operation with innovative ”dry” cooling.

The FemtoLux femtosecond laser has a tunable pulse duration from <400 fs to 1 ps and can operate in a broad AOM controlled range of pulse repetition rates from a single shot to 4 MHz.

The maximum pulse energy is 1 mJ operating with single pulses and can reach even up to 2 mJ in burst mode, ensuring higher ablation rates and processing throughput for different materials.

The FemtoLux beam parameters will meet the requirements of the most demanding materials and micro-machining applications.

Innovative laser control electronics ensure simple control of the FemtoLux laser by external controllers that could run on different platforms, be it Windows, Linux or others using REST API commands.

This makes easy integration and reduces the time and human resources required to integrate this laser into any laser micromachining equipment.

Material processing examples made with FemtoLux laser

Material processing examples made with FemtoLux laser.

Courtesy of FTMC and Femtika.

Seamless user experience

  • Easy integration – remote control using REST API via RS232 and LAN.
  • Reduced integration time – demo electronics is available for laser control programming in advance.
  • Easy and quick installation – no water, fully disconnectable laser head. Can be installed by the end-user.
  • Easy troubleshooting – integrated detectors and constant system status logging.
  • No periodic maintenance required.

Direct Refrigerant Cooling (DRC)

“Dry“ Cooling

Direct refrigerant cooling is industry-proven thermal-management approach with a long history in everyday technologies such as domestic refrigeration and automotive climate control. Unlike conventional liquid cooling, it operates without pumped water circuits, relying instead on direct refrigerant-based heat transfer.

Benefits

  • Military-grade reliability 90 000 hours MTBF
  • No maintenance
  • 50 % lower power consumption compared to water cooling equipment
  • Easy and simple installation
  • Increased stability due to precise temperature control across a wide range of operating conditions
  • “Greenest” cooling technology

How DRC Works

At its core, DRC eliminates the inherent reliability limitations of water-based cooling loops. Rather than circulating liquid coolant through pumps, hoses, and reservoirs, refrigerant is delivered directly to a cold plate that is in contact to the laser head.

The FemtoLux cooling architecture comprises four key elements: a compressor, condenser, expansion valve, and evaporator. High-pressure refrigerant is circulating through the expansion valve, which is mounted directly on the cooling plate. As the refrigerant expands, it enters the plate as a low-temperature, low-pressure liquid. While flowing through the plate, it absorbs heat from the laser head and undergoes a controlled phase change into vapor. This vapor is then compressed and routed through the condenser, where heat is released to the surrounding environment and the refrigerant returns to liquid form.

The closed refrigerant circuit provides exceptional integration flexibility. The compressor and condenser are housed within the power supply unit, while the cooling plate and expansion valve are connected via three‑meter armored flexible lines. This arrangement allows the laser head to be installed inside material processing workstations or mounted on moving stages. A variable-speed compressor continuously adjusts cooling output to match real-time thermal demand, preventing temperature fluctuations that can affect laser performance.

DRC layout

Straightforward Installation and Maintenance-Free Operation

For ease of integration, the cooling plate can be detached from the laser head during system assembly. Flexible refrigerant lines allow the laser head to be positioned independently of the compressor unit, simplifying mechanical integration.

Because the refrigerant loop is hermetically sealed at the factory, routine maintenance associated with water-based systems – such as refilling, filter changes, or system flushing – is eliminated entirely.

For system integrators, dry cooling represents a substantial step forward. By removing the constraints of water and air cooling, DRC simplifies system design while enabling compact layouts. The streamlined cold-plate interface reduces installation complexity, and the compact power supply unit supports straightforward system integration.

The absence of pumps and reservoirs keeps system dimensions small. The compressor is up to 10 times smaller and lighter than conventional designs. The FemtoLux laser head with integrated cooling plate weighs 32 kg, while the power supply unit – including compressor and condenser – adds only 15 kg.

Precision Temperature Control and Energy Efficiency

FemtoLux 30 and 50 power consumption and output power comparison versus other ultrafast lasers manufacturers

Direct refrigerant cooling delivers approximately 50% higher energy efficiency than water-cooled solutions, while maintaining highly uniform cold-plate temperatures through phase-change heat transfer. Comparative testing has shown that DRC systems consume roughly half the electrical power of traditional liquid chillers under identical operating conditions.

Thermal regulation is both precise and responsive. The variable-speed compressor adapts continuously to changing heat loads, maintaining laser operating temperature within ±0.1 °C across the full performance range.

FemtoLux lasers use a low–global-warming-potential (GWP) refrigerant approved for laboratory operation and transport. Compared to alternative cooling methods, DRC consumes about half the power of chiller-based systems and up to eight times less than thermoelectric cooling solutions. Unlike air cooling, DRC can operate below ambient temperature or hold a tightly defined thermal setpoint.

Proven Reliability from Military to Industry

This cooling approach has been deployed by Aspen Systems for more than 15 years in demanding defense applications where size, weight, efficiency, and reliability are critical. These include military communications systems, high-power directed-energy platforms on armored vehicles, transport enclosures, ships, and helicopters.

The technology demonstrates a mean time between failures (MTBF) exceeding 90,000 hours, enabling continuous operation for more than a decade. In long-term testing, FemtoLux lasers have demonstrated stable operation beyond 25,000 hours. Compressor service life typically surpasses that of water-chiller pumps by a factor of three to five, further enhancing system reliability.

Aspen refigeration systems, as used in military applications

Dry cooling technology developed by EKSPLA engineers is featured as the cover story in the November, 2025 issue of Photonics Spectra, the industry’s leading magazine with the largest worldwide circulation in lasers, optics, and photonics.

Specifications

ModelFemtoLux 30FemtoLux 50FemtoLux HE
Main Specifications 1)
Central wavelength1030 nm1030 nm1030 nm
Laser pulse repetition rate (PRR) 2)200 kHz – 2 MHz,
4 MHz optional
100 kHz – 2 MHz,
4 MHz optional
10 kHz – 1 MHz
Pulse picker PRRLaser PRR / N, N=1, 2, 3, … , 65000; single shotLaser PRR / N, N=1, 2, 3, … , 65000; single shotLaser PRR / N, N=1, 2, 3, … , 65000; single shot
Maximal average output power 3)≥ 30 W≥ 45 W (typical 50 W)≥ 30 W
Pulse energy 4)≥ 100 µJ, 300 µJ optional≥ 250 µJ (typical 300 µJ)1 mJ
Power long term stability (Std. dev.) 5)< 0.5 %< 0.5 %< 0.5 %
Pulse energy stability (Std. dev.) 6)< 1 %< 1 %< 1 %
Pulse duration (FWHM) @ 1 MHz 7)< 400 fs – 1 ps< 400 fs – 1 ps< 400 fs – 1 ps
Number of pulses in MHz burst 8)2 – 102 – 102 – 10
Total energy in burst mode 9)> 450 µJ> 750 µJ2 mJ
Beam qualityM2 < 1.2 (typical < 1.1)M2 < 1.2 (typical < 1.1)M2 < 1.3
Beam ellipticity, far field0.85 (typical ≥ 0.9)0.85 (typical ≥ 0.9)0.85 (typical ≥ 0.9)
Beam divergence (full angle)< 1 mrad< 1 mrad< 1 mrad
Beam pointing thermal stability< 20 µrad/°C< 20 µrad/°C< 20 µrad/°C
Beam diameter (1/e2)2.5 ± 0.4 mm @ 65 cm2.5 ± 0.4 mm @ 65 cm2.5 ± 0.4 mm @ 65 cm
Polarizationverticalverticalvertical
Synchronization modeinternal / externalinternal / externalinternal / external
Pulse output controlfrequency divider, pulse picker, burst mode, packet triggering, power attenuation, pulse-on-demandfrequency divider, pulse picker, burst mode, packet triggering, power attenuation, pulse-on-demandfrequency divider, pulse picker, burst mode, packet triggering, power attenuation, pulse-on-demand
Control interfacesRS232 / LANRS232 / LANRS232 / LAN
Length of the umbilical cord3 m, detachable3 m, detachable3 m, detachable
Laser head cooling typedry (direct refrigerant cooling through detachable cooling plate), water cooling optionaldry (direct refrigerant cooling through detachable cooling plate), water cooling optionaldry (direct refrigerant cooling through detachable cooling plate), water cooling optional
Physical characteristics
Laser head (W × L × H)434 × 569 × 150 mm434 × 569 × 150 mm434 × 569 × 150 mm
Power supply unit (W × L × H)483 × 534 × 184 mm483 × 534 × 184 mm483 × 534 × 184 mm
Operating Requirements
Mains requirements100 – 240 V AC, single phase, 50/60 Hz100 – 240 V AC, single phase, 50/60 Hz100 – 240 V AC, single phase, 50/60 Hz
Maximal power rating1000 W1000 W1000 W
Operating ambient temperature18 – 27 °C18 – 27 °C18 – 27 °C
Relative humidity10 – 80 % (non-condensing)10 – 80 % (non-condensing)10 – 80 % (non-condensing)
Air contamination levelISO 9 (room air) or betterISO 9 (room air) or betterISO 9 (room air) or better
ModelFemtoLux 30FemtoLux 50FemtoLux HE
  1. Due to continuous improvement, all specifications are subject to change without notice. Parameters marked typical are not specifications. They are indications of typical performance and will vary with each unit we manufacture. All parameters are specified for a shortest pulse duration. Unless stated otherwise, all specifications are measured at 1030 nm and for basic system without options.
  2. When frequency divider is set to transmit every pulse. Fully controllable by integrated AOM.
  3. At 1 MHz. Please see graphs for power vs laser pulse repetition rate of FemtoLux series lasers.
  4. For FemtoLux 30 maximal pulse energy 300 µJ at 50 kHz. Standard energy 100 µJ at 200 kHz.
  5. Over 100 h after warm-up under constant environmental conditions.
  6. Under constant environmental conditions.
  7. Please see graph for typical pulse duration for different repetition rates.
  8. Oscillator frequency ~50 MHz, ~20 ns separation between pulses.
  9. For MHz burst mode or MHz+GHz burst mode at 50 kHz PRR. For Femtolux HE at 10 kHz.

Harmonics modules

Central wavelength515 nm343 nm
Main specifications 1) 2)
Pulse energy 3)50 µJ30 µJ
Average powerup to 25 Wup to 10 W
Beam qualityM2 < 1.2M3 < 1.3
Beam ellipticity, far field> 0.85> 0.85
Beam divergence (full angle)< 0.7 mrad< 0.5 mrad
Beam diameter (1/e2)2.2 ± 0.4 mm @ 30 cm2.4 ± 0.4 mm @ 30 cm
Physical characteristics
Laser head with harmonic module (W × L × H)434 × 747 × 158 mm434 × 747 × 158 mm
Central wavelength515 nm343 nm
  1. Due to continuous improvement, all specifications are subject to change without notice. Parameters marked typical are not specifications. They are indications of typical performance and will vary with each unit we manufacture. All parameters are specified for a shortest pulse duration.
  2. Harmonics are optimized at shortest pulse duration and 100 µJ pulse energy. For optimization at different pulse duration or energy, please inquire sales@ekspla.com.
  3. Please see graphs for power vs laser pulse repetition rate graphs of FemtoLux series lasers.

GHz burst option

Main specifications 1)
Laser Pulse Repetition Rate (PRR)up to 500 kHz
Intra-burst pulse repetition rate 2)2 ± 0.25 GHz
GHz burst modeshortlong
GHz burst length0.5 – 10 ns20 – 500 ns
Number of pulses 3)2 – 2040 – 1000
Shapesquare, rising, fallingfalling, pre-shaped 3)
MHz + GHz Burst Mode
Number of pulses in MHz burst2 – 10
Number of pulses in GHz burst 4)2 – 20
  1. Due to continuous improvement, all specifications are subject to change without notice. Parameters marked typical are not specifications. They are indications of typical performance and will vary with each unit we manufacture. All parameters are specified for a shortest pulse duration.
  2. Custom intra-pulse PRR is available upon a request.
  3. Depends on the intra-pulse PRR.
  4. For more information, please inquire sales@ekspla.com.

Benefits

  • Jitter lower than 20 ns ensures consistent and equidistant pulse spacing for high-speed micromachining
  • Adjustable repetition rate for processing complex geometries
  • Faster processing speeds, increased productivity

PoD feature enables the laser to fire a pulse only when required, rather than at a constant rate, enabling precise control over the laser’s output and resulting in higher efficiency, accuracy and quality.

This capability is especially valuable in various micromachining applications where a high processing speed, constant energy, and accuracy are essential. To follow complex curvature at high speed and to maintain equidistant spacing it is necessary to ensure that the repetition rate of the pulses is adjusted. To achieve these requirements, it is necessary to ensure that the repetition rate of the pulses is adjusted to follow complex curvature at high speed and to maintain equidistant spacing. One may try to use position based laser triggering but, due to laser system limitations, the jitter will be from several μs to tens of μs, which will result in random spacing of the pulses.

On the other hand, the usage of time based laser triggering results in overheat areas, due to excessive overlap of pulses. The FemtoLux laser has the pulse-on-demand feature with jitter as low as 20 ns (peak-to-peak), and it can therefore tackle all the challenges and maximize process efficiency, precision and quality at high speed.

Traditional laser triggering techniques struggle to maintain equally spaced pulses at high speeds (Fig.1, 2). Pulse-on-demand feature tackles this challenge and enables high-speed micromachining (Fig. 3).

Benefits

  • Any desired intra-burst PRR can be achieved independently from the initial PRR of the master oscillator
  • Identical pulse separation inside the GHz bursts is maintained
  • Short- and long-burst formation modes can be provided.
    – A short burst is up to about 10 ns burst width (from 2 to tens of pulses in the GHz burst).
    – A long burst is from ~20 ns up to a few hundred ns in burst width (from tens to thousands of pulses in the GHz burst)
  • MHz+GHz burst mode
  • An adjustable amplitude envelope of the GHz bursts is provided
  • No pre/post pulses in GHz burst. Pure GHz bursts
  • Ultrashort pulse duration is maintained inside the bursts

Patent-Pending Method

The Femtolux laser can operate in the single-pulse mode, MHz burst mode, GHz burst mode, and MHz + GHz burst mode.

The burst formation technique based on the use of the AFL is a very versatile method as it allows to overcome many limitations encountered by other fiber- and/or solid-state-based techniques.

A new versatile patent-pending method to form ultra-high repetition rate bursts of ultrashort laser pulses. The developed method is based on the use of an all-in-fiber active fiber loop (AFL). A detailed description of the invention can be found on:

  1. Tadas Bartulevičius, Mykolas Lipnickas, Virginija Petrauskienė, Karolis Madeikis, and Andrejus Michailovas, (2022), “30 W-average-power femtosecond NIR laser operating in a flexible GHz‑burst-regime,” Opt. Express 30, 36849-36862. DOI: 10.1364/OE.472907.
  2. Andrejus Michailovas, and Tadas Bartulevičius. 2021 Int. patent application published under the Patent Cooperation Treaty (PCT) WO2021059003A1.

Short GHz burst

Long GHz burst

MHz + GHz burst mode

FemtoLux 50 performance

FemtoLux HE performance

FemtoLux 30 performance

FemtoLux 30 stability

Drawings

Laser control application

Ekspla Control Application is a software tool intended for day-to-day routine operation control. It is used to control the laser in API level through LAN or RS-232 communication types, the control capabilities are stored in the laser system itself, software is self-adaptive to the system, one application can be used with multiple systems and can run on different platforms – be it Windows, Linux or others using REST API commands.

Laser control application

Applications

More applications

Publications

Formation of through-glass vias (TGVs) in glass substrates using femtosecond laser operating in MHz/GHz burst mode

D. Andriukaitis, V. Stankevič, E. Kažukauskas, and P. Gečys, in Lasers in Manufacturing Conference 2025, (WLT, 2025).

In Transition from Battlefield to Industry, Dry Laser Cooling Makes a Splash

L. Ūkanis, D. Andriukaitis, L. Rimgaila, and J. Burnett, Photonics Spectra 59 (11), 43-48 (2025).

Polarization-Dependent Laser-Assisted Cutting of Glass Using a Nondiffractive Beam in the MHz Burst Regime

J. Dudutis, A. Kondratas, and P. Gečys, ACS Photonics 12 (7), 3706-3716 (2025). DOI: 10.1021/acsphotonics.5c00679.

Comparative analysis of microlens array formation in fused silica glass by laser: Femtosecond versus picosecond pulses

L. Zubauskas, E. Markauskas, A. Vyšniauskas, V. Stankevič, and P. Gečys, Journal of Science: Advanced Materials and Devices 9 (4), 100804 (2024). DOI: 10.1016/j.jsamd.2024.100804.

The ultrafast burst laser ablation of metals: Speed and quality come together

A. Žemaitis, U. Gudauskytė, S. Steponavičiūtė, P. Gečys, and M. Gedvilas, Optics & Laser Technology 180, 111458 (2024). DOI: 10.1016/j.optlastec.2024.111458.

Ultrashort Pulse Bursts for Surface Laser Polishing

S. Steponavičiūtė, P. Gečys, G. Račiukaitis, M. Gedvilas, and A. Žemaitis, in Optics, Photonics and Lasers OPAL’ 2024 Conference Proceedings, S. Y. Yurish, ed. (IFSA Publishing, 2024), pp. 44.

Femtosecond Laser Cutting of 110 – 550 µm Thickness Borosilicate Glass in Ambient Air and Water

E. Markauskas, L. Zubauskas, G. Račiukaitis, and P. Gečys, Micromachines 14 (1) (2023). DOI: 10.3390/mi14010176.

GaAs ablation with ultrashort laser pulses in ambient air and water environments

E. Markauskas, L. Zubauskas, A. Naujokaitis, B. Čechavičius, M. Talaikis, G. Niaura et al., Journal of Applied Physics 133 (23), 235102 (2023). DOI: 10.1063/5.0152173.

Laser-generated nanoparticles from Fe-based metallic glass in water and its amorphization control by pulsed laser processing

S. Liang, M. E. R. Reusmann, K. Loza, S. Zerebecki, L. Zhang, Z. Jia et al., Materials Today Chemistry 30, 101544 (2023). DOI: 10.1016/j.mtchem.2023.101544.

Versatile ultrashort pulse laser tunable up to nanosecond range

T. Bartulevičius, M. Lipnickas, K. Madeikis, R. Burokas, and A. Michailovas, in Solid State Lasers XXXII: Technology and Devices, W. A. Clarkson, and R. K. Shori, eds. (SPIE, 2023), pp. 1239904. DOI: 10.1117/12.2649867.

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