Atlantic
High Power Industrial Picosecond Lasers
High-energy and high-power water-cooled Atlantic series picosecond lasers are designed for a variety of material processing applications in R&D labs.
Features
- At 1064 nm
Up to 80 W output power, up to 200 μJ pulse energy - At 532 nm (optional)
Up to 40 W output power, up to 100 μJ pulse energy - At 355 nm (optional)
Up to 30 W output power, up to 75 μJ pulse energy - Up to 1 MHz repetition rate
- Short pulse duration 10 ps
- M²<1.3
- Versatile laser control and syncronisation capabilities
- Smart triggering for synchronous operation with polygon scanner and PSO
- Monolythic, sealed and rugged design
- Low ownership cost
- Nanosecond pulse duration mode (optional)
Applications
- Drilling
- Cutting
- Patterning
- Structuring
- Ablation
- Dicing
- Micromachining
- LCD, OLED cutting
- Laser induced forward transfer
- Sapphire structuring and dicing
- Ceramics micromachining
- PCD drilling and tracing
- Silicon scribing
- PET, PP, PTFE, Silicone cutting and drilling
Description
High-energy and high-power water-cooled Atlantic series picosecond lasers are designed for a variety of industrial applications.
Suitable for LCD or OLED display cutting and drilling, laser induced forward transfer (LIFT), glass and sapphire processing, micromachining of ultra-hard materials, ablation of metals, cutting and drilling of polymers, silicon scribing, solar cell scribing and many more.
Superior beam quality parameters, maximum available average power (80 W @ IR / 40 W @ VIS / 30 W @ UV), maximum available pulse energy (200 μJ @ IR / 100 μJ @ VIS / 75 μJ @ UV) and maximum pulse repetition rate (up to 1 MHz) are beneficial where high processing quality and high throughput are required.
To tailor laser performance for specific industrial applications, advanced electronics enable external gating (including PSO), synchronization and precise laser triggering as well as instant signal amplitude control.
To maintain reliability and assure long-term stable operation in an industrial environment, optical components are installed in a sealed, robust, precisely machined monolithic aluminum block. Designed for robust, low maintenance operation, Atlantic series lasers offer maximum reliability due to an optimized layout, PC controlled operation, a built-in self-diagnostic system and advanced status reporting.
To tailor laser performance for specific industrial applications, advanced electronics enable external gating (including PSO), synchronization and precise laser triggering as well as instant signal amplitude control.
To maintain reliability and assure long-term stable operation in an industrial environment, optical components are installed in a sealed, robust, precisely machined monolithic aluminum block. Designed for robust, low maintenance operation, Atlantic series lasers offer maximum reliability due to an optimized layout, PC controlled operation, a built-in self-diagnostic system and advanced status reporting.
For industrial high-power UV laser applications, high reliability and low ownership cost of UV components is crucial. To meet these requirements, the optical layouts of Atlantic UV models are optimized for longevity and stable operation in the UV range, resulting in a UV optics lifetime of 8,000 hours.
A unique optional feature of Atlantic high-power lasers is that they can work in both picosecond and nanosecond modes. This 2-in-1 laser solution is beneficial for some materials processing (such as glass or ceramics), where both very high accuracy, low processed surface roughness and high throughput are required at low cost.
Specifications
Model | Atlantic 50 | Atlantic 80 |
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Main Specifications 1) | ||
Central wavelength | ||
Fundamental | 1064 nm | 1064 nm |
With 2H option | 532 nm (optional 1064 nm output) 2) | 532 nm (optional 1064 nm output) 2) |
With 3H option | 355 nm (optional 1064 nm and/or 532 nm outputs) 2) | 355 nm (optional 1064 nm and/or 532 nm outputs) 2) |
Laser pulse repetition rate (PRRL) range 3) | 300 – 1000 kHz | 400 – 1000 kHz |
Pulse repetition rate after frequency divider | PRR = PRRL / N, N=1, 2, 3, … , 1025 | PRR = PRRL / N, N=1, 2, 3, … , 1025 |
Maximal average output power 4) | ||
At 1064 nm | 50 W | 80 W |
At 532 nm | 25 W | 40 W |
At 355 nm | 18 W | 30 W |
Pulse energy at lowest PRRL 4) | ||
At 1064 nm | 165 µJ | 200 µJ |
At 532 nm | 85 µJ | 100 µJ |
At 355 nm | 60 µJ | 75 µJ |
Pulse contrast | ||
At 1064 nm | > 300 : 1 | > 300 : 1 |
At 532 nm | > 500 : 1 | > 500 : 1 |
At 355 nm | > 1000 : 1 | > 1000 : 1 |
Power long term stability over 8 h (Std. dev.) 5) | < 1.0 % | < 1.0 % |
Pulse energy stability (Std. dev.) 6) | ||
At 1064 nm | < 1.0 % | < 1.0 % |
At 532 nm | < 2.0 % | < 2.0 % |
At 355 nm | < 2.5 % | < 2.5 % |
Pulse duration (FWHM) at 1064 nm | 10 ± 3 ps | 10 ± 3 ps |
Polarization | linear, vertical 100 : 1 | linear, vertical 100 : 1 |
M2 | < 1.3 | < 1.3 |
Beam circularity, far field | > 0.85 | > 0.85 |
Beam divergence, full angle | < 1.5 mRad | < 1.5 mRad |
Beam pointing stability (pk-to-pk) 7) | < 50 µRad | < 50 µRad |
Beam diameter (1/e2) at 50 cm distance from laser aperture | ||
At 1064 nm | 1.8 ± 0.3 mm | 1.8 ± 0.3 mm |
At 532 nm | 1.8 ± 0.3 mm | 2.2 ± 0.3 mm |
At 355 nm | 1.8 ± 0.3 mm | 2.0 ± 0.3 mm |
Triggering mode | internal / external | internal / external |
Pulse output control | frequency divider, pulse picker, instant amplitude control, power attenuation | frequency divider, pulse picker, instant amplitude control, power attenuation |
Control interfaces | keypad / USB / RS232 / LAN | keypad / USB / RS232 / LAN |
Physical characteristics | ||
Cooling | water | water |
Laser head size (L×W×H) | ||
Single output 1064 nm | 396 × 173 × 755 mm | 396 × 173 × 755 mm |
Single output 355 nm | 396 × 173 × 1000 mm | 396 × 173 × 1000 mm |
3 outputs 1064 / 532 / 355 nm | 396 × 173 × 926 mm | 396 × 173 × 926 mm |
Power supply unit size (L×W×H) | 553 × 1019 × 852 mm | 553 × 1019 × 852 mm |
Umbilical length | 4 m | 4 m |
Operating Requirements | ||
Mains requirements | 100 – 240 V AC, single phase 47 – 63 Hz | 100 – 240 V AC, single phase 47 – 63 Hz |
Maximal power consumption | < 3.1 kW | < 3.5 kW |
Operating ambient temperature | 18 – 27 °C | 18 – 27 °C |
Relative humidity | 10 – 80 % (non-condensing) | 10 – 80 % (non-condensing) |
Air contamination level | ISO 9 (room air) or better | ISO 9 (room air) or better |
Classification | ||
Classification according EN60825-1 | CLASS 4 laser product | CLASS 4 laser product |
Model | Atlantic 50 | Atlantic 80 |
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- 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.
- Can be ordered either in a single output or in 2 or 3 separate harmonics outputs versions.
- When frequency divider is set to transmit every pulse.
- See typical power and energy curves for other pulse repetition rates.
- At the lowest PRRL after warm-up under constant environmental conditions.
- At the lowest PRRL under constant environmental conditions.
- Beam pointing stability is evaluated as a movement of the beam centroid in the focal plane of a focusing element.
Performance
Stability
Drawings
Publications
Laser-generated nanoparticles from Fe-based metallic glass in water and its amorphization control by pulsed laser processing
The laser synthesis and processing of colloids represents a group of scalable and “green” synthesis methods of crystalline metal oxides, that have recently made encouraging progresses in preparing amorphous as well as defect-rich nanoparticles. The relevant conditions and mechanisms that allow the design of amorphous metal oxides (AMOs) remain unknown. Consequently, in this work the synthesis of Fe-based partially amorphous oxide nanoparticles (NPs) by pulsed laser ablation in water was studied. Furthermore, both laser pulse duration and the number of laser pulse in pulsed laser fragmentation in liquid (LFL) allow a precise control of amorphization of AMOs in water. Hereby, a high-fluence nanosecond-LFL provides a significantly higher amorphization rate, whereas picosecond-LFL always presents minor fractions of crystalline α-Fe even with a higher specific energy input and laser intensity. Consequently, the laser fluence required for the repeated melting and quenching of NP appears to be the decisive parameter to control amorphization. During laser synthesis and processing of colloids, the amorphization of AMOs appears to be linked to the apparent size reduction effect, while a complete full amorphization of AMOs may be attributed to the stronger oxidation effects. This work will stimulate future studies using laser-generated AMO NPs for further functional purposes.
Thermal control of SZ2080 photopolymerization in four-beam interference lithography
Photopolymerization by four-beam interference lithography on a preheated SZ2080 sample was explored at different initial temperatures of the sample: 20 °C, 50 °C, 75 °C, 100 °C, 125 °C, and 150 °C, and at exposure times ranging from 0.5 s to 5 s. The average laser power selected was ∼100 mW for the 300 ps duration pulses at a 1 kHz repetition rate. The experimental results demonstrate that the higher initial temperature of the sample positively influences the crosslinking of the patterns. These findings will improve polymerization protocols for multi-beam interference lithography.
Glass dicing with elliptical Bessel beam
In this paper the possibility to optimize the glass dicing process by controlling the axicon-generated Bessel beam ellipticity is presented. Single-shot intra-volume modifications in soda-lime glass followed by dicing experiments of 1 mm-thick samples are performed. The Bessel beam ellipticity is essential for glass dicing process. Such beam generates intra-volume modifications with transverse crack propagation in dominant direction. Orientation of these modifications parallel to the dicing direction gives significant advantages in terms of processing speed, glass breaking force and cutting quality.
High-efficiency laser fabrication of drag reducing riblet surfaces on pre-heated Teflon
Bio-inspired surfaces are able to decrease friction with fluids and gases. The most recognizable are shark-skin-like riblet surface structures. Such bio-inspired surfaces can be formed by the laser ablation technique. In this work, bio-inspired riblet surfaces with grooves were formed using picosecond ultraviolet laser ablation on pre-heated polytetrafluoroethylene (PTFE) at various sample temperatures. The ablation of hot PTFE was found to be 30% more efficient than the conventional laser structuring at the room temperature. The friction of structured PTFE surfaces with the flowing air was investigated by using drag a measurement setup. Results show the decrease of friction force by 6% with dimensionless riblet spacing around 14–20.
Laser-Ablated Silicon in the Frequency Range From 0.1 to 4.7 THz
The optical performance of high-resistivity silicon with a laser-ablated surface was studied in the transmission mode in the frequency range of 0.1-4.7 THz. A reciprocal relationship between the transmission brightness and the surface roughness was observed at discrete THz frequencies. The measured dispersion was reproduced by the THz wave scattering theory using an effective refractive index model. No significant differences between the samples processed either with psor ns-duration laser pulses in ambient air or in argon enriched atmosphere were found in the THz regime. It was demonstrated that the majority of optical losses of the silicon with the laser modified surface were due to the scattering of THz waves and not due to the absorption in silicon-compounds formed during the laser ablation.
Laser-assisted selective copper deposition on commercial PA6 by catalytic electroless plating – Process and activation mechanism
Results of in-depth experimental analysis of the laser-assisted local copper deposition on commercial Polyamide 6 (PA 6) are presented. Pico- and nanosecond lasers were validated for surface modification of the polymer followed by silver (I) activation and finished by autocatalytic electroless copper plating on the laser-modified areas. Detailed investigations were dedicated to finding out the origin of selective metal plating, including the surface profiling and wettability dynamics, XPS analysis and electric resistance measurements of the deposited copper layer. Based on the experimental data, the mechanism of the polymer surface activation by the laser modification is proposed.
Mechanism of pillars formation using four-beam interference lithography
Three different experiments were performed in order to determine the mechanism of pillars formation using four-beam interference lithography. The experimental results demonstrate that pillars, fabricated in argon gas, were wider and higher compared with the pillars fabricated in nitrogen gas, low vacuum or air. It clearly indicates that the pillar bottom widening effect is not affected by the depletion of atmospheric oxygen as in all environments the fabricated pillars have a wider bottom part. Moreover, the shape of the fabricated pillars is not affecting by the back reflection from the positioning stage and by the light irradiation conditions. These results clearly indicate that the photopolymerization process is enhanced by the heat current and it determines the pillar bottom widening effect.
Raising the maximum power density of nanoporous catalyst film-based polymer-electrolyte-membrane fuel cells by laser micro-machining of the gas diffusion layer
Although nanoporous Pt film has been shown to be an effective catalyst for polymer electrolyte membrane (PEM) fuel cells, the maximum power density of the cell is limited by the optimal film thickness. When the Pt film thickness exceeds the optimal value, regions with good gas transport (the side near the gas diffusion layer (GDL)) separate from regions with good proton transport (the side near the PEM), so the current density and the power density drop with increasing film thickness. Here we demonstrate that this obstacle can be overcome by laser micro-machining the GDL. The picosecond laser fabricates grooves on the GDL surface to greatly increase the effective surface area for Pt deposition, thereby reducing the local Pt film thickness. A nearly two-fold increase in the power density is achieved by using laser micro-machined periodic grooves of 20 μm depth, reaching a 0.6-V power density of 853 mW cm−2 and a maximum power density of 1.2 W cm−2 with a cathode Pt loading of 200 μg cm−2. The results also indicate that further enhancement may be achieved by increasing the surface modulation depth/period ratio and by implementing a better way to fill the grooves with polymer electrolyte.
Rapid high-quality 3D micro-machining by optimised efficient ultrashort laser ablation
Solid-state lasers with pulse duration of 10 ps and radiation wavelength of 1064 nm were used to investigate the laser ablation efficiency dependence on processing parameters: laser fluence (pulse energy and beam spot size), beam scanning speed, pulse repetition rate, and scanned line (hatch) distance for the copper sample. Utilising a 40 W power laser, the highest ablation efficiency of 2.5 µm3/µJ and the ablation rate of 100 µm3/µs with the smallest surface roughness of 0.2 µm was obtained. Three-dimensional (3D) fabrication using a galvanometer scanner and layer-by-layer removal technique with optimal parameters defined for efficient ablation were demonstrated at a rate of 6 mm3/min. Combination of high material removal rate with excellent quality and complex 3D structure formation is in a high interest for mimicking bio-inspired surfaces, micro-mould fabrication and decorative applications.
Thermochemical writing with high spatial resolution on Ti films utilising picosecond laser
In this paper, we investigate the local oxidation of titanium thin films under the action of picosecond laser pulses. Periodical structures were recorded by the multi-beam interference scheme utilizing various numbers of laser beams, and the relationship between spatial resolution and the contrast of the structures was studied. The Raman spectra of the laser processing regions confirmed the oxidation even under the action of a single picosecond pulse. An analytical simulation of titanium film oxidation in the interference field was provided, and obtained results are correlated with the experimental data. The results of theoretical modeling show that the thermochemical effects of picosecond laser pulses allow recording periodic structures with a period of 0.65 lines per μm. The demonstrated results are important in the adaptation of technological laser systems for the manufacture of diffractive optical elements.