Modular-Design Industrial-Grade Femtosecond Lasers PHAROS Lasers
- 190 fs – 20 ps tunable pulse duration
- 2 mJ maximum pulse energy
- 20 W maximum output power
- Single-shot – 1 MHz repetition rate
- Pulse picker for pulse-on-demand mode
- Industrial-grade design
- Optional automated harmonic generator
- Optional CEP stabilization
- Optional repetition rate locking to an external source
Features
- 190 fs – 20 ps tunable pulse duration
- 2 mJ maximum pulse energy
- 20 W maximum output power
- Single-shot – 1 MHz repetition rate
- Pulse picker for pulse-on-demand mode
- Industrial-grade design
- Optional automated harmonic generator
- Optional CEP stabilization
- Optional repetition rate locking to an external source
PHAROS is a series of femtosecond lasers combining millijoule pulse energy and high average power. PHAROS features a mechanical and optical design optimized for both scientific and industrial applications. A compact, thermally-stabilized, and sealed design enables PHAROS integration into various optical setups and machining workstations. Diode-pumped Yb medium significantly reduces maintenance costs and provides a long laser lifetime, while the robust optomechanical design enables stable operation in varying environments.
The tunability of PHAROS allows the system to cover applications normally requiring multiple different laser systems. Tunable parameters include pulse duration (190 fs – 20 ps), repetition rate (single-shot – 1 MHz), pulse energy (up to 2 mJ), and average power (up to 20 W). A pulse-on-demand mode is available using the built-in pulse picker. The versatility of PHAROS can be extended by a variety of optional modules.
- More models are available on request.
- Assuming Gaussian pulse shape.
- Precise wavelengths for specific models are available on request.
- FWHM, measured at laser output, using maximum pulse energy.
- Under stable environmental conditions.
- Normalized to average pulse energy, NRMSD.
- Custom spacing is available on request.
- Maximum number of pulses in a burst depends on the laser repetition rate. Custom number of pulses are available on request.
- Dimensions might increase for the lasers with integrated optional modules.
Near-field (a) and far-field (b)
Pump: 10 W, 100 µJ, 100 kHz
Pump: 10 W, 100 µJ, 100 kHz
PHAROS lasers have an option for tunable GHz and MHz burst with burst-in-burst capability – called BiBurst. In standard mode, a single pulse is emitted at some fixed frequency. In burst mode, the output consists of pulse packets instead of single pulses. Each packet consists of a certain number of equally separated pulses. MHz‑Burst contains N pulses with a nanosecond period, GHz‑Burst contains P pulses with a picosecond period. If both bursts are used, the equally separated pulse packets contain sub‑packets of pulses (burst‑in‑burst, BiBurst).
PHAROS lasers equipped with automated harmonic generators (HGs) provide a selection of fundamental (1030 nm), second (515 nm), third (343 nm), fourth (257 nm), or fifth (206 nm) harmonic outputs using software control. HGs are perfect for industrial applications that require a single-wavelength output. Modules, mounted directly at the output of the laser, are fully integrated into the system.
The industrial-grade optical parametric amplifier I-OPA series marks a new era of simplicity in the world of tunable wavelength femtosecond light sources. Based on over 10 years of experience producing the ORPHEUS series of optical parametric amplifiers, this solution brings together the tunability of wavelength with the robust industrial-grade design. The I-OPA is a rugged module attachable to PHAROS lasers, providing long-term stability comparable to that of the industrial-grade harmonic generators.
PHAROS lasers can be equipped with feedback electronics for carrier-envelope phase (CEP) stabilization of the output pulses. The carrier-envelope offset (CEO) of the PHAROS oscillator is actively locked to 1/4th of the repetition rate with a < 100 mrad standard deviation. The CEP stable pulses from the synchronized amplifier have a < 350 mrad standard deviation. The CEP drift occurring inside the amplifier and the user’s setup can be compensated with an out of loop f-2f interferometer, which is a part of the complete PHAROS active CEP stabilization package.
The oscillator of PHAROS laser can be customized for repetition rate locking applications. Coupled with the necessary feedback electronics, the repetition rate is synchronized to an external RF source using the two piezo stages installed inside the cavity. The repetition rate locking system can assure an integrated timing jitter of less than 200 fs for RF reference frequencies larger than 500 MHz. Continuous phase shifting is available on request.
All-optical sampling of few-cycle infrared pulses using tunneling in a solid
Y. Liu, S. Gholam‑Mirzaei, J. E. Beetar, J. Nesper, A. Yousif, M. Nrisimhamurty, and M. Chini, Photonics Research 6 (9), 929 (2021).
An ultrafast vibrational study of dynamical heterogeneity in the protic ionic liquid ethyl-ammonium nitrate. I. Room temperature dynamics
C. A. Johnson, A. W. Parker, P. M. Donaldson, and S. Garrett‑Roe, The Journal of Chemical Physics 13 (154), 134502 (2021).
Biodegradable Harmonophores for Targeted High-Resolution In Vivo Tumor Imaging
A. Y. Sonay, K. Kalyviotis, S. Yaganoglu, A. Unsal, M. Konantz, C. Teulon, I. Lieberwirth, S. Sieber, S. Jiang, S. Behzadi et al., ACS Nano 3 (15), 4144-4154 (2021).
Birefringent optical retarders from laser 3D-printed dielectric metasurfaces
S. Varapnickas, S. C. Thodika, F. Moroté, S. Juodkazis, M. Malinauskas, and E. Brasselet, Applied Physics Letters 15 (118), 151104 (2021).
Charge photogeneration and recombination in ternary polymer solar cells based on compatible acceptors
R. Hu, W. Zhang, Z. Xiao, J. Zhang, X. Su, G. Wang, J. Chen, X. He, and R. Wang, Journal of Materials Science 25 (56), 14181-14195 (2021).
Comparison of growth interruption and temperature variation impact on emission efficiency in blue InGaN/GaN MQWs
J. Mickevičius, K. Nomeika, M. Dmukauskas, A. Kadys, S. Nargelas, and R. Aleksiejūnas, Vacuum 183, 109871 (2021).
Direct correlation of local fluence to single-pulse ultrashort laser ablated morphology
H. Sakurai, K. Konishi, H. Tamaru, J. Yumoto, and M. Kuwata‑Gonokami, Communications Materials 1 (2) (2021).
Direct Femtosecond Laser Fabrication of Chemically Functionalized Ultra-Black Textures on Silicon for Sensing Applications
Y. Borodaenko, S. Gurbatov, M. Tutov, A. Zhizhchenko, S. A. Kulinich, A. Kuchmizhak, and A. Mironenko, Nanomaterials 2 (11), 401 (2021).
Direct imaging of electric field behavior in 2,7-diphenyl[1]benzothieno[3,2-b][1]benzothiophene organic field-effect transistors by sum-frequency generation imaging microscopy
C. Katagiri, T. Miyamae, H. Li, F. Yang, and S. Baldelli, Physical Chemistry Chemical Physics 8 (23), 4944-4950 (2021).
Direct Laser Writing for the Formation of Large-Scale Gold Microbumps Arrays Generating Hybrid Lattice Plasmon Polaritons in Vis–NIR Range
E. Stankevičius, K. Vilkevičius, M. Gedvilas, E. Bužavaitė‑Vertelienė, A. Selskis, and Z. Balevičius, Advanced Optical Materials, 2100027 (2021).
PHAROS Modular-Design Industrial-Grade Femtosecond Lasers
Product datasheet.
Rev. 21/04/2021. Size 790 KB.
I-OPA Industrial-Grade Optical Parametric Amplifier
Product datasheet.
Rev. 21/08/2021. Size 516 KB.
Tunable GHz and MHz Burst with Burst-in-Burst Capability
Product datasheet.
Rev. 18/02/2021. Size 95 KB.
Related products
Thank you for reaching out!
We appreciate you contacting LIGHT CONVERSION.
We will get back in touch with you as soon as possible.
Something went wrong.
We are sorry for the inconvenience, please send your request to sales@lightcon.com
Done