Wavelength-Tunable Sources for Yb Lasers

The highlight of wavelength-tunable sources is the ORPHEUS series of femtosecond optical parametric amplifiers (OPAs) for Yb lasers. ORPHEUS series enables operation at high repetition rates while maintaining the best properties of TOPAS series OPAs such as the wide tuning range from deep-UV to mid-IR and high output stability. Coupled with PHAROS or CARBIDE femtosecond laser, ORPHEUS makes an invaluable source for ultrafast spectroscopy, nonlinear microscopy, and a variety of other scientific applications. The latest addition, ORPHEUS-NEO, is a next generation OPA with exceptional stability and is equipped with multiple detectors for pump beam position tracking and continuous monitoring of output parameters; thus, it is an invaluable tool for the most demanding applications.

The list of wavelength-tunable sources also includes I-OPA, a compact industrial-grade OPA, and CRONUS-3P, an OPA-based ultrafast source with GDD control for advanced nonlinear microscopy. For more information on the latter, refer to microscopy systems.

Platforms
  ORPHEUS ORPHEUS-NEO I-OPA / CRONUS-3P TOPAS
  Ytterbium (Yb)
Ti:Sapphire
Automated wavelength tunability + + + +
Single-box solution     +  
Continuous power monitoring and diagnostics   +    

Pump beam position tracking

  +    
Fully integrated wavelength extensions   + +  
Environmentally sealed for higher stability   + +  

 

ORPHEUS Comparison Table
Product 1) Max. pump power Pump pulse energy Tuning range Extended tuning range Pulse duration Special features
HP 80 W 20 – 800 µJ 640 – 1010 nm, 1050 – 2600 nm  320 – 2600 nm 120 – 250 fs

Continuous power monitoring and diagnostics

Exceptional output stability

ONE 1350 – 2000 nm, 2100 – 4500 nm 640 – 16000 nm 100 – 300 fs
HP 80 W 8 – 400 μJ 630 – 2600 nm 190 – 16000 nm 120 – 250 fs Fully automated
HE 400 – 2000 μJ High energy
80 W 10 – 500 μJ 650 – 900 nm, 1200 – 2500 nm 325 – 2500 nm 25 – 100 fs 2) Optional GDD control 
HP 80 W 12 – 400 μJ 1350 – 2000 nm, 2100 – 4500 nm 1350 – 2000 nm, 2100 – 16000 nm 100 – 300 fs Fully automated
HE 400 – 2000 μJ High energy
80 W 200 – 2000 μJ 2500 – 10000 nm 1350 – 15000 nm < 100 fs Broad-bandwidth mid-IR output
20 W 200 – 1000 μJ 320 – 900 nm 250 – 300 nm,
320 – 900 nm
< 50 fs Ultrashort UV – VIS – NIR output
2H 8 W 10 – 200 μJ 650 – 900 nm 325 – 450 nm, 650 – 900 nm < 30 fs @ 700 – 850 nm Broad-bandwidth output
3H 8 W 12 – 200 μJ 520 – 900 nm 260 – 450 nm, 520 – 900 nm < 30 fs @ 530 – 670 nm
60 W 16 – 2000 μJ 630 – 4500 nm 3) 210 – 16000 nm 3) Down to < 40 fs 3) Two independent outputs
20 W 100 – 3200 μJ 640 – 1000 nm, 1060 – 2600 nm 210 – 4800 nm 1 – 3 ps Narrow-bandwidth output 
  1. Custom solutions are available; contact sales@lightcon.com for details.
  2. Typical. Long pulse mode is also available; see detailed specifications.
  3. Depends on configuration. Choose between ORPHEUSORPHEUS-F, and ORPHEUS-ONE configurations.
I-OPA Comparison Table
Product 1) Max. pump power Pump pulse energy Tuning range Extended tuning range Pulse duration Special features
I-OPA logo TW 1) HP 40 W 10 – 400 µJ 640 – 1010 nm,
1050 – 2600 nm
320 – 2600 nm 120 – 250 fs

Compact industrial-grade design

High output stability

F 650 – 900 nm,
1200 – 2500 nm
– 2) 25 – 100 fs
ONE 20 – 400 µJ 1350 – 2000 nm, 2100 – 4500 nm 1350 – 10000 nm 100 – 300 fs
  1. Fixed-wavelength models (I-OPA-FW) are also available; see specifications.
  2. Contact sales@lightcon.com for information.
  • Wavelength tunability in an industrial design
  • Single-box solution
  • Tunable or fixed-wavelength models
  • Plug-and-play installation and robust performance
  • The most compact OPA in the market
  • From UV to MIR
  • Continuous power monitoring and diagnostics
  • Pumped by PHAROS-UP for ultrashort pulses
  • Up to 80 W, 800 µJ pump at up to 2 MHz
  • Fully integrated wavelength extensions
  • Second repetition rate pump option
  • Exceptional output stability
  • Continuous tunability from UV to MIR, 190 – 16000 nm
  • High energy and high power models for all needs
  • Single-shot – 2 MHz repetition rate
  • Up to 80 W pump power
  • Up to 2 mJ pump pulse energy
  • Combination of best collinear and non-collinear OPA features
  • Ultrashort pulses in NIR (650 – 900 nm and 1200 – 2500 nm)
  • Single-shot – 2 MHz repetition rate
  • < 100 fs pulse duration
  • Adjustable spectral bandwidth
  • Optional long pulse mode for gap-free tunability
  • High conversion efficiency in MIR, 1350 – 16000 nm
  • High energy and high power models for all needs
  • Single-shot – 2 MHz repetition rate
  • Up to 80 W pump power
  • Up to 2 mJ pump pulse energy
  • Broad-bandwidth MIR pulses at high repetition rate
  • Continuously tunable in 2500 – 15 000 nm range
  • Short-pulse high-energy auxiliary output at 2000 nm
  • Pumped by industrial-grade lasers for high stability
  • CEP-stable option
  • Ultrashort UV – VIS – NIR output
  • < 50 fs pulse duration at 500 nm
  • Up to 100 kHz repetition rate
  • Up to 20 W, 1 mJ pump
  • Optional UV extension down to 250 nm
  • NOPA for the shortest tunable pulses
  • Pulse duration down to < 30 fs
  • Integrated prism compressor
  • Adjustable spectral bandwidth and pulse duration
  • Wavelength feedback with internal spectrometer
  • Two simultaneous independently tunable outputs
  • 210 – 16000 nm tuning range
  • Single-shot – 2 MHz repetition rate
  • Up to 60 W, 0.5 mJ pump
  • Compact and cost-effective
  • CEP-stable option
  • Picosecond pulses from femtosecond pump
  • 210 – 4800 nm tuning range
  • 800 fs – 3 ps pulse duration
  • < 20 cm-1 spectral bandwidth
  • Up to 100 kHz repetition rate
  • High output stability
  • Tunable pulse duration, 100 fs – 20 ps
  • Maximum pulse energy of up to 4 mJ
  • Down to < 100 fs right at the output
  • Pulse-on-demand and BiBurst for pulse control
  • Up to 5th harmonic or tunable extensions
  • CEP stabilization or repetition rate locking
  • Thermally-stabilized and sealed design
  • Tunable pulse duration, 190 fs – 20 ps
  • Maximum output of 80 W and 2 mJ
  • Single-shot – 2 MHz repetition rate
  • Pulse-on-demand and BiBurst for pulse control
  • Up to 5th harmonic or tunable extensions
  • Air-cooled model
  • Compact industrial-grade design

Broadband Multidimensional Spectroscopy Identifies the Amide II Vibrations in Silkworm Films

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Charge Photogeneration and Recombination in Fluorine-Substituted Polymer Solar Cells

R. Hu, Y. Liu, J. Peng, J. Jiang, M. Qing, X. He, M. Huo, and W. Zhang, Frontiers in Chemistry 10 (2022).

Cobalt(III) Carbene Complex with an Electronic Excited-State Structure Similar to Cyclometalated Iridium(III) Compounds

N. Sinha, B. Pfund, C. Wegeberg, A. Prescimone, and O. S. Wenger, Journal of the American Chemical Society 22 (144), 9859-9873 (2022).

Deep tissue multi-photon imaging using adaptive optics with direct focus sensing and shaping

Z. Qin, Z. She, C. Chen, W. Wu, J. K. Y. Lau, N. Y. Ip, and J. Y. Qu, Nature Biotechnology (2022).

Dopamine Photochemical Behaviour under UV Irradiation

A. Falamaş, A. Petran, A. Hada, and A. Bende, International Journal of Molecular Sciences 10 (23), 5483 (2022).

Effects of polyethylene oxide particles on the photo-physical properties and stability of FA-rich perovskite solar cells

R. K. Koech, Y. A. Olanrewaju, R. Ichwani, M. Kigozi, D. O. Oyewole, O. V. Oyelade, D. M. Sanni, S. A. Adeniji, E. Colin‑Ulloa, L. V. Titova et al., Scientific Reports 1 (12) (2022).

Electron–Hole Binding Governs Carrier Transport in Halide Perovskite Nanocrystal Thin Films

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Enhanced transfer efficiency of plasmonic hot-electron across Au/GaN interface by the piezo-phototronic effect

Y. Zhu, C. Deng, C. He, W. Zhao, Z. Chen, S. Li, K. Zhang, and X. Wang, Nano Energy 93, 106845 (2022).

Evidence and Governing Factors of the Radical-Ion Photoredox Catalysis

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Exciton-Like and Mid-Gap Absorption Dynamics of PtS in Resonant and Transparent Regions

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