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Amplified Lasers

 fs-Version or ns-Version Tunable pulse duration Customer specific pulse parameters or seed laser  GHz operation  Burst mode operation External pulse compression with MPC or HCF for few cycles pulses SHG, THG, HHG generation

Specifications

Center Wavelength: 1030 nm
Repetition Rate: 1 – 1000 kHz
Pulse Energy: 300 mJ
Energy Stability (RMS): 1 %
Pulse Duration: 100 fs
The Indylit 20 is the highest average power and most efficient passively air-cooled femtosecond laser on the market. If you need a reliable femtosecond laser that is maintenance-free, turn-key, and has exquisite optical parameters – look no further! The laser features an innovative and patented passive cooling design, ensuring ...

Specifications

Center Wavelength: 1030 nm
Repetition Rate: 100 – 1000 kHz
Pulse Energy: 0.13 mJ
Energy Stability (RMS): 1 %
Pulse Duration: 400 fs
The Indylit 20 is the highest average power and most efficient passively air-cooled femtosecond laser on the market. If you need a reliable femtosecond laser that is maintenance-free, turn-key, and has exquisite optical parameters – look no further! The laser features an innovative and patented passive cooling design, ensuring ...

Specifications

Center Wavelength: 515 nm
Repetition Rate: 100 – 1000 kHz
Pulse Energy: 0.07 mJ
Energy Stability (RMS): 2 %
Pulse Duration: 400 fs
The NeoVan™ Ultra-Compact Diode Laser Module represents a breakthrough in laser technology, offering unparalleled performance in an incredibly compact form factor. Engineered with precision and reliability in mind, this diode laser module is ideal for a wide range of demanding applications where stability, precision, and beam ...

Specifications

Center Wavelength: 1064 nm
Repetition Rate: Not Specified
Pulse Energy: 5 mJ
Energy Stability (RMS): 1 %
Pulse Duration: Not Specified
The neoYb Amplifier Module represents a cutting-edge solution in solid-state laser technology, designed to significantly boost pulse energy or average output power across a wide range of laser applications. With its innovative design and advanced features, this amplifier module offers exceptional performance, reliability, and ...

Specifications

Center Wavelength: 1030 nm
Repetition Rate: Not Specified
Pulse Energy: 0.5 mJ
Energy Stability (RMS): Not Specified
Pulse Duration: 700 fs
This is an ultracompact ultrafast amplifier/booster from Skynet Lasers. SkyAMP - 1030 nm - LP integrates Skynet Lasers\' proprietary SkyAmp engine rendering an ultracompact footprint that will be an ideal choice as a standalone system or an additional staging booster in a larger setup. This miniature ...

Specifications

Center Wavelength: 1030 nm
Repetition Rate: Not Specified
Pulse Energy: 1 mJ
Energy Stability (RMS): 1 %
Pulse Duration: 500 fs
The neoMOS Picosecond Laser series offers a compact and powerful solution for industrial laser applications. Combining state-of-the-art picosecond oscillators with a solid-state amplifier, this laser system provides high stability and long lifetime for 24/7 industrial use. With a ultra-compact laser head design and customizable ...

Specifications

Center Wavelength: 1064 nm
Repetition Rate: 0.001 – 40000 kHz
Pulse Energy: 0.25 mJ
Energy Stability (RMS): 1 %
Pulse Duration: 10000 fs
Indylit 10 is high energy air-cooled laser suitable for a variety of ultrafast applications. The laser head features an entirely passively-cooled design (patent pending), ensuring high stability of the optical parameters such as pulse duration, beam pointing and power. Its mechanical construction can withstand almost ...

Specifications

Center Wavelength: 1030 nm
Repetition Rate: 100 – 1600 kHz
Pulse Energy: 0.1 mJ
Energy Stability (RMS): 1 %
Pulse Duration: 400 fs
Indylit 10 is high energy air-cooled laser suitable for a variety of ultrafast applications. The laser head features an entirely passively-cooled design (patent pending), ensuring high stability of the optical parameters such as pulse duration, beam pointing and power. Its mechanical construction can withstand almost everything you ...

Specifications

Center Wavelength: 515 nm
Repetition Rate: 100 – 1600 kHz
Pulse Energy: 0.05 mJ
Energy Stability (RMS): 2 %
Pulse Duration: Not Specified
The PL2230 series is a family of high-performance Diode Pumped Solid-State (DPSS) picosecond Nd:YAG lasers, designed to deliver exceptional pulse energies and precise pulse durations in the picosecond range. These mode-locked lasers are ideal for various applications in time-resolved fluorescence, spectroscopy, laser-induced ...

Specifications

Center Wavelength: 1064 nm
Repetition Rate: 0.05 – 0.1 kHz
Pulse Energy: 3 mJ
Energy Stability (RMS): 0.5 %
Pulse Duration: 28000 fs
The SkyAMP system 2000 nm is an ultra-fast laser amplifier system integrating the SkyAmp engine, This can be used as an amplifier or as a booster. Easy in-line integration with USB interface.

Specifications

Center Wavelength: 2000 nm
Repetition Rate: Not Specified
Pulse Energy: 1 mJ
Energy Stability (RMS): 1 %
Pulse Duration: 100 fs
The Huaray-Olive series, High-Power Picosecond Ultra-fast Lasers (50W@1064nm) is a compact and powerful, hybrid fiber/free space amplified Ultra-fast laser. With pulses shorter than 10ps, this laser is ideal for fast, high precision micro-machining and material processing of any material. The robust laser combines the advantages of ...

Specifications

Center Wavelength: 1064 nm
Repetition Rate: 200 – 1000 kHz
Pulse Energy: 0.1 mJ
Energy Stability (RMS): 3 %
Pulse Duration: 10000 fs
Olive Mid-power Picosecond Laser is a product newly launched specific to micro machining marketby North America Ultra-fast R&D center established by Huaray after purchasing Canadian Attodyne. The product is pushed out by combining advanced of the R&D Center and excellent process optimization and batch delivery capability of ...

Specifications

Center Wavelength: 1064 nm
Repetition Rate: 0.001 – 1000 kHz
Pulse Energy: 0.06 mJ
Energy Stability (RMS): 3 %
Pulse Duration: 10000 fs
Olive Mid-power Picosecond Laser is a product newly launched specific to micro machining marketby North America Ultra-fast R&D center established by Huaray after purchasing Canadian Attodyne. The product is pushed out by combining advanced of the R&D Center and excellent process optimization and batch delivery capability of ...

Specifications

Center Wavelength: 532 nm
Repetition Rate: 100 – 500 kHz
Pulse Energy: 0.05 mJ
Energy Stability (RMS): 3 %
Pulse Duration: 10000 fs
The Huaray-Olive series, Low-power Picosecond Ultra-fast Lasers (4W@532nm, 10W@1064nm), Robust and affordable, it produces high energy pulses with durations below 10 ps. The laser is based on a hybrid optical amplifier architecture that combines the advantages of fiber laser technology with solid state diode pumped multi-pass ...

Specifications

Center Wavelength: 1064 nm
Repetition Rate: 50 – 1000 kHz
Pulse Energy: 0.02 mJ
Energy Stability (RMS): 3 %
Pulse Duration: 10000 fs
The Huaray-Olive series, Low-power Picosecond Ultra-fast Lasers (4W@532nm, 10W@1064nm), Robust and affordable, it produces high energy pulses with durations below 10 ps. The laser is based on a hybrid optical amplifier architecture that combines the advantages of fiber laser technology with solid state diode pumped multi-pass ...

Specifications

Center Wavelength: 532 nm
Repetition Rate: 50 – 300 kHz
Pulse Energy: 0.4 mJ
Energy Stability (RMS): 3 %
Pulse Duration: 10000 fs

Ultrafast Laser Amplifiers: Powering Precision in Science and Industry

Ultrafast laser amplifiers are specialized optical systems designed to enhance ultrashort laser pulses—typically in the femtosecond (fs) or picosecond (ps) range—by increasing their energy and peak power without compromising their temporal characteristics. These amplifiers are pivotal in applications requiring high-intensity, short-duration light pulses, such as nonlinear optics, material processing, and advanced imaging techniques.

Operating Principles

The core mechanism behind ultrafast amplifiers is Chirped Pulse Amplification (CPA). In this process, an initial ultrashort pulse is temporally stretched to reduce its peak power, making it suitable for amplification without damaging the gain medium. The stretched pulse is then amplified in a gain medium, such as titanium-doped sapphire (Ti:sapphire) or ytterbium-doped fiber, before being recompressed to its original duration. This technique allows for significant energy increase while preserving the pulse's ultrashort nature.

Types of Ultrafast Amplifiers

  1. Regenerative Amplifiers: These devices use a feedback loop to amplify the pulse multiple times within the gain medium, achieving high energy levels with relatively low pump power.

  2. Multipass Amplifiers: In these systems, the pulse passes through the gain medium multiple times in a single pass, enhancing energy gain without the need for complex feedback mechanisms.

  3. Fiber Amplifiers: Utilizing optical fibers doped with rare-earth elements, fiber amplifiers offer high efficiency and excellent beam quality, making them suitable for high-repetition-rate applications.

  4. Optical Parametric Amplifiers (OPAs): OPAs use nonlinear crystals to amplify pulses through parametric processes, enabling tunable wavelength generation.

Applications

  • Materials Processing: Ultrafast amplifiers are employed in precision micromachining, laser ablation, and surface structuring, where high peak powers are necessary to achieve fine resolution without thermal damage.

  • Medical Imaging: In techniques like multiphoton microscopy, ultrafast lasers provide the necessary resolution and tissue penetration for deep-tissue imaging.

  • Spectroscopy: Time-resolved spectroscopy, including pump-probe experiments, relies on ultrafast amplifiers to study dynamic processes on femtosecond timescales.

  • Fundamental Research: High-intensity ultrafast lasers are used in exploring nonlinear optical phenomena, attosecond science, and high-field physics.

Recent Developments

Advancements in ultrafast amplifier technology have led to systems with higher repetition rates and improved beam quality. For instance, the development of high-power ytterbium-doped fiber amplifiers has enabled average powers exceeding 3.5 kW while maintaining excellent beam quality. Additionally, innovations in optical parametric amplification have facilitated tunable ultrafast sources across a broad spectral range, enhancing versatility in various applications.

Conclusion

Ultrafast laser amplifiers are indispensable tools in modern science and industry, enabling the generation of high-energy, short-duration light pulses for a myriad of applications. Ongoing research and technological advancements continue to push the boundaries of what is achievable, opening new frontiers in ultrafast science and engineering.

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.