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.

Download datasheet

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
  • High energy version available (1 mJ at 10 kHz)
  • > 750 µJ in a burst mode
  • < 350 fs – 1 ps
  • Pulse duration extension up to 1 ns
  • Single shot 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 circularity > 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 <350 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 more than 300 μJ operating with single pulses and can reach more than 750 µJ 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.

Innovative “Dry” Cooling System

Direct refrigerant cooling system compressor

Direct refrigerant cooling system compressor.

Picture courtesy of Aspen Systems Inc.

The FemtoLux laser employs an innovative cooling system and sets new reliability standards among industrial femtosecond lasers. No additional bulky and heavy water chiller is needed.

The chiller requires periodic maintenance – cooling system draining and rinsing and water and particle filter replacement. Moreover, water leakage can cause damage to the laser head and other equipment. Instead of using water for transferring heat from a laser head, the FemtoLux laser uses an innovative Direct Refrigerant Cooling method.

The refrigerant agent circulates from a PSU-integrated compressor and condenser, to a cooling plate via armored flexible lines.

The entire cooling circuit is permanently hermetically sealed and requires no maintenance.

Direct refrigerant cooling system features

  • Military-grade reliability
  • Permanently hermetically sealed system >90,000 hour MTBF
  • No maintenance
  • High cooling efficiency
  • >45% lower power consumption compared to water cooling equipment
  • Compact and light

Simple & reliable cooling plate attachment

The cooling plate is detachable from the laser head for more convenient laser installation. The laser cooling equipment is integrated with the laser power supply unit into a single 4U rack-mounted housing with a total weight of 15 kg.

Specifications

ModelFemtoLux 30FemtoLux 50
Main Specifications 1)
Central wavelength
Fundamental1030 nm1030 nm
With second harmonic option515 nm515 nm
With third harmonic option343 nm343 nm
Pulse Repetition Rate (PRR) 2)200 kHz – 4 MHz100 kHz – 2 MHz
Pulse repetition frequency (PRF) after frequency dividerPRF = PRR / N, N=1, 2, 3, … , 65000; single shotPRF = PRR / N, N=1, 2, 3, … , 65000; single shot
Average output power
At 1030 nm 3)> 27 W (typical 30 W)> 45 W (typical 50 W)
At 515 nm> 11 W 4)> 20 W 5)
At 343 nm> 6 W 4)> 10 W 5)
Pulse energy
At 1030 nm> 100 µJ or 1 mJ 6)> 300 µJ 7)
At 515 nm> 55 µJ 4)> 50 µJ 5)
At 343 nm> 30 µJ 4)> 25 µJ 5)
Number of pulses in MHz burst 8)2 – 102 – 10
Total energy in burst mode 9)> 450 µJ> 750 µJ
Power long term stability (Std. dev.) 10)< 0.5 %< 0.5 %
Pulse energy stability (Std. dev.) 11)< 1 %< 1 %
Pulse duration (FWHM) @ 1 MHzTunable, < 350 fs 12) – 1 ps 13)Tunable, < 400 fs 12) – 1 ps 13)
Optional pulse duration extensiontunable, up to 1 nstunable, up to 1 ns
Beam qualityM2 < 1.2 (typical < 1.1)M2 < 1.2 (typical < 1.1)
Beam circularity, far field> 0.85> 0.85
Beam divergence (full angle)< 1 mrad< 1 mrad
Beam pointing thermal stability< 20 µrad/°C< 20 µrad/°C
Beam diameter (1/e2) at 1030 nm2.5 ± 0.4 mm @ 65 cm2.5 ± 0.4 mm @ 65 cm
Polarizationverticalvertical
Triggering modeinternal / externalinternal / external
Pulse output controlfrequency divider, pulse picker, burst mode, packet triggering, power attenuation, pulse-on-demand 14)frequency divider, pulse picker, burst mode, packet triggering, power attenuation, pulse-on-demand 14)
Control interfacesRS232 / LANRS232 / LAN
Length of the umbilical cord3 m, detachable3 m, detachable
Laser head cooling typedry (direct refrigerant cooling through detachable cooling plate)dry (direct refrigerant cooling through detachable cooling plate)
Physical characteristics
Laser head (W × L × H)434 × 569 × 150 mm434 × 569 × 150 mm
Power supply unit (W × L × H)449 × 496 × 177 mm449 × 496 × 177 mm
Operating Requirements
Mains requirements100 – 240 V AC, single phase, 50/60 Hz100 – 240 V AC, single phase, 50/60 Hz
Maximal power rating800 W800 W
Operating ambient temperature18 – 27 °C18 – 27 °C
Relative humidity10 – 80 % (non-condensing)10 – 80 % (non-condensing)
Air contamination levelISO 9 (room air) or betterISO 9 (room air) or better
ModelFemtoLux 30FemtoLux 50
  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.
  4. At 200 kHz.
  5. At 400 kHz.
  6. Other combinations of energy and repetition rate available.
  7. At 100 kHz.
  8. Oscillator frequency ~50 MHz, ~20 ns separation between pulses.
  9. MHz burst mode or MHz+GHz burst mode at 50 kHz PRR.
  10. Over 100 h after warm-up under constant environmental conditions.
  11. Under constant environmental conditions.
  12. At PRR > 500 kHz. At PRR < 500 kHz shortest pulse duration is < 400 fs.
  13. Custom pulse duration by request. For example – fixed 50 fs available.
  14. Optional feature. Jitter < 20 ns. Trigger-to-pulse delay < 1 µs.

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 for Ultra-High Rate Bursts

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.

Specifications

Main Specifications
Burst repetition rateup to 650 kHz
Intra-burst pulse repetition rate 1)2 GHz
GHz Burst Modeshortlong
GHz burst length0.5 – 10 ns20 – 500 ns
Number of pulses 2)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 2)2 – 20
  1. Custom intra-pulse PRR is available upon a request.
  2. Depends on the intra-pulse PRR.
  3. For more information, please inquire sales@ekspla.com.

FemtoLux 50 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.

Publications

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.

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.

30 W-average-power femtosecond NIR laser operating in a flexible GHz-burst-regime

T. Bartulevicius, M. Lipnickas, V. Petrauskiene, K. Madeikis, and A. Michailovas, Opt. Express 30 (20), 36849-36862 (2022). DOI: 10.1364/OE.472907.

Spatially Variable Wave Plate for Depolarization Compensation Induced in High-Power Yb:YAG Amplifier

R. Burokas, O. Ulčinas, K. Michailovas, R. Danilevičius, A. Kazakevičius, and A. Michailovas, in Conference on Lasers and Electro-Optics, (Optica Publishing Group, 2022), pp. JW3A.58. DOI: 10.1364/CLEO_AT.2022.JW3A.58.

Depolarization compensation with a spatially variable wave plate in a 116  W, 441  fs, 1  MHz Yb:YAG double-pass laser amplifier

L. Veselis, R. Burokas, O. Ulčinas, T. Gertus, K. Michailovas, and A. Michailovas, Appl. Opt. 60 (24), 7164-7171 (2021). DOI: 10.1364/AO.432573.

EKSPLA: Reliability redefined: a new 30W femtosecond laser with zero maintenance

A. Juronis, in SPIE Exhibition Product Demonstrations, C. Chair, ed. (SPIE, 2021), pp. 117160J.

Numerical model of end-pumped Yb:YAG double-pass laser amplifier experimentally validated at 129 W output power

L. Veselis , R. Burokas , and A. Michailovas , Lithuanian Journal of Physics 61 (4) (2021). DOI: 10.3952/physics.v61i4.4641 .

1

2

Content not found