Broad-Bandwidth Hybrid Optical Parametric Amplifier ORPHEUS-F

  • 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

Features

  • 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

ORPHEUS-F is a hybrid optical parametric amplifier (OPA), combining the short pulse duration produced by a non‑collinear OPA (NOPA) and the wide tuning range offered by a collinear OPA.

The Signal pulses of ORPHEUS-F are tunable in a 650 – 900 nm range and can be compressed with a simple prism-based compressor down to 25 – 70 fs pulse duration. The Idler pulses are tunable in a 1200 – 2500 nm range and reach pulse duration of 40 – 100 fs. In addition, a long-pulse mode is available for accessing the 900 – 1200 nm tuning range; thus, enabling a gap-free tunability.

ORPHEUS-F provides significantly shorter pulses compared to the standard ORPHEUS model and a wider tuning range compared to the non-collinear ORPHEUS-N. Thus, for many scientific applications, ORPHEUS-F is the optimal choice.

For compact single-box solution, refer to I-OPA in ORPHEUS-F configuration.

Model ORPHEUS‑F
Mode of operation Short pulse mode 1) Long pulse mode
Tuning range 650 – 900 nm (Signal)
1200 – 2500 nm (Idler)
650 – 1010 nm (Signal)
1050 – 2500 nm (Idler)
Maximum pump power 80 W
Pump pulse energy 10 – 500 µJ
Conversion efficiency 2) > 7% @ 700 nm
Integrated 2H (515 nm) generation efficiency 3) > 35 %
Pulse duration before compression 1) < 290 fs
Spectral bandwidth 200 – 750 cm-1 @ 650 – 900 nm 75 – 220 cm-1 @ 650 – 900 nm
Pulse duration after compressor 1) < 55 fs @ 800 – 900 nm
< 70 fs @ 650 – 800 nm
< 100 fs @ 1200 – 2000 nm
n/a
Compressor transmission > 65% @ 650 – 900 nm
> 80% @ 1200 – 2000 nm
Long-term power stability, 8h 4) < 2% @ 800 nm
Pulse-to-pulse energy stability, 1 min 4) < 2% @ 800 nm
  1. In short pulse mode, broadband pulses are compressed externally. Typical pulse duration before compression: 120 – 250 fs, after compression: 25 – 70 fs @ 650 – 900 nm, 40 – 100 fs @ 1200 – 2000 nm.
  2. Specified as percentage of pump power, before compressor. Conversion efficiency at peak is equal to 10% for signal and idler combined.
  3. At designated output port; not simultaneous to OPA output.
  4. Expressed as NRMSD (normalized root mean squared deviation).
Model ORPHEUS‑F
Mode of operation Short pulse mode Long pulse mode
325 – 450 nm (SHS) > 1% n/a
325 – 505 nm (SHS) n/a > 1%
525 – 650 nm (SHI) > 0.5%
600 – 650 nm (SHI) > 0.5% n/a
210 – 252 nm (FHS) n/a > 0.1%
263 – 325 nm (FHI) > 0.1%
2500 – 15000 nm See ORPHEUS-MIR
  1. For > 15 µJ pump pulse energy.
Model ORPHEUS-F
Pump laser PHAROS or CARBIDE
Center wavelength 1030 ± 10 nm
Maximum pump power  80 W
Repetition rate Single-shot – 2 MHz
Pump pulse energy 10 – 500 μJ
Pulse duration 1) 180 – 300 fs
  1. FWHM, assuming Gaussian pulse shape.
Model ORPHEUS-F
Operating temperature 1) 19 – 25 ºC (air conditioning recommended)
Relative humidity 1) 20 – 70% (non-condensing)
Electrical requirements 100 – 240 V AC, 1.4 A; 50 – 60 Hz
Rated power 120 W
Power consumption Standby: 10 W
Max during wavelength tuning: 100 W
  1. Specifications are guaranteed for a maximum temperature variation of ± 1 ºC and humidity variation of ± 10%.

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).

Highly nonlinear dipolar exciton-polaritons in bilayer MoS2

B. Datta, M. Khatoniar, P. Deshmukh, F. Thouin, R. Bushati, S. D. Liberato, S. K. Cohen, and V. M. Menon, Nature Communications 1 (13) (2022).

Direct focus sensing and shaping for high-resolution multi-photon imaging in deep tissue

Z. Qin, Z. She, C. Chen, W. Wu, J. K. Y. Lau, N. Y. Ip, and J. Y. Qu, (2021).

Germanium-lead perovskite light-emitting diodes

D. Yang, G. Zhang, R. Lai, Y. Cheng, Y. Lian, M. Rao, D. Huo, D. Lan, B. Zhao, and D. Di, 1 (12) (2021).

In-vivo tracking of harmonic nanoparticles: a study based on a TIGER widefield microscope [Invited]

L. Vittadello, C. Kijatkin, J. Klenen, D. Dzikonski, K. Kömpe, C. Meyer, A. Paululat, and M. Imlau, Optical Materials Express 7 (11), 1953 (2021).

NIR-to-NIR Imaging: Extended Excitation Up to 2.2 µm Using Harmonic Nanoparticles with a Tunable hIGh EneRgy (TIGER) Widefield Microscope

L. Vittadello, J. Klenen, K. Koempe, L. Kocsor, Z. Szaller, and M. Imlau, Nanomaterials 12 (11), 3193 (2021).

Nonlinear optical properties of 6H-SiC and 4H-SiC in an extensive spectral range

X. Guo, Z. Peng, P. Ding, L. Li, X. Chen, H. Wei, Z. Tong, and L. Guo, Optical Materials Express 4 (11), 1080 (2021).

Recrystallization of CsPbBr3 Nanoparticles in Fluoropolymer Nonwoven Mats for Down- and Up-Conversion of Light

V. Neplokh, D. I. Markina, M. Baeva, A. M. Pavlov, D. A. Kirilenko, I. S. Mukhin, A. P. Pushkarev, S. V. Makarov, and A. A. Serdobintsev, Nanomaterials 2 (11), 412 (2021).

The Multiple Roles of Metal Ion Dopants in Spectrally Stable, Efficient Quasi-2D Perovskite Sky-Blue Light-Emitting Devices

C. H. A. Li, P. Geng, S. B. Shivarudraiah, M. Ng, X. Zhang, B. Xu, L. Guo, and J. E. Halpert, , 2100860 (2021).

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