Non-Collinear Optical Parametric Amplifier ORPHEUS-N

  • < 30 fs pulse duration
  • Single-shot – 1 MHz repetition rate
  • Integrated prism compressor
  • Adjustable spectral bandwidth and pulse duration
  • Wavelength feedback with internal spectrometer

Features

  • < 30 fs pulse duration
  • Single-shot – 1 MHz repetition rate
  • Integrated prism compressor
  • Adjustable spectral bandwidth and pulse duration
  • Wavelength feedback with internal spectrometer

ORPHEUS-N is a non-collinear optical parametric amplifier (NOPA). Depending on the ORPHEUS-N model, it has a built‑in second or third harmonic generator producing a 515 nm or 343 nm pump, respectively. ORPHEUS-N with a second harmonic pump (ORPHEUS-N-2H) delivers pulses of less than 30 fs in the 700 – 850 nm range. ORPHEUS-N with a third harmonic pump (ORPHEUS-N-3H) delivers pulses of less than 30 fs in the 530 – 670 nm range. ORPHEUS-N works at repetition rates of up to 1 MHz.

An optional second harmonic generator is available, extending the tuning range down to 260 – 450 nm. Featuring a built-in pulse compressor, ORPHEUS-N is an invaluable instrument for time-resolved spectroscopy. A single PHAROS or CARBIDE laser can pump more than one OPA device providing several pump and/or probe channels with independent wavelength tuning.

Model ORPHEUS‑N‑2H ORPHEUS‑N‑3H
Tuning range 650 – 900 nm (Signal) 520 – 900 nm (Signal)
Integrated 2H / 3H generation efficiency > 35% (515 nm) > 25% (343 nm)
Maximum pump power 8 W
Pump pulse energy 10 – 200 µJ 12 – 200 µJ
Conversion efficiency at peak 700 nm 800 nm 580 nm 700 nm 800 nm
> 7 % > 5 % > 1.3 % > 0.7 % > 0.3 %
Pulse duration after compressor < 30 fs (700 – 850 nm) < 30 fs (530 – 670 nm)
< 80 fs (670 – 900 nm)
Long-term power stability, 8 h 1) < 2% @ 800 nm < 2% @ 580 nm
Pulse-to-pulse energy stability, 1 min 1) < 2% @ 800 nm < 2% @ 580 nm
  1. Expressed as NRMSD (normalized root mean squared deviation).
Model ORPHEUS‑N‑2H ORPHEUS‑N‑3H
Tuning range (SHS) 325 – 450 nm 260 – 450 nm
Conversion efficiency at peak > 10% of Signal
Model ORPHEUS‑N‑2H ORPHEUS‑N‑3H
Pump laser PHAROS or CARBIDE
Center wavelength 1030 ± 10 nm
Maximum pump power 8 W
Repetition rate Single-shot – 800 kHz Single-shot – 600 kHz
Pump pulse energy 10 – 200 μJ 12 – 200 μJ
Pulse duration 1) 180 – 300 fs
  1. FWHM, assuming Gaussian pulse shape.

Manipulating Crystallization Kinetics of Conjugated Polymers in Nonfullerene Photovoltaic Blends toward Refined Morphologies and Higher Performances

J. Zhan, L. Wang, M. Zhang, L. Zhu, T. Hao, G. Zhou, Z. Zhou, J. Chen, W. Zhong, C. Qiu et al., Macromolecules 9 (54), 4030-4041 (2021).

Momentarily trapped exciton polaron in two-dimensional lead halide perovskites

W. Tao, C. Zhang, Q. Zhou, Y. Zhao, and H. Zhu, Nature Communications 1 (12) (2021).

Strained Epitaxy of Monolayer Transition Metal Dichalcogenides for Wrinkle Arrays

J. Wang, M. Han, Q. Wang, Y. Ji, X. Zhang, R. Shi, Z. Wu, L. Zhang, A. Amini, L. Guo et al., ACS Nano (2021).

Ultrafast generation and decay of a surface metal

L. Gierster, S. Vempati, and J. Stähler, Nature Communications 1 (12) (2021).

Vibrational coherent control of localized d–d electronic excitation

A. Marciniak, S. Marcantoni, F. Giusti, F. Glerean, G. Sparapassi, T. Nova, A. Cartella, S. Latini, F. Valiera, A. Rubio et al., Nature Physics (2021).

A combined laser-based angle-resolved photoemission spectroscopy and two-photon photoemission spectroscopy study of Td–WTe2

P. Hein, S. Jauernik, H. Erk, L. Yang, Y. Qi, Y. Sun, C. Felser, and M. Bauer, Journal of Physics: Condensed Matter 34 (32), 345503 (2020).

Isoenergetic two-photon excitation enhances solvent-to-solute excited-state proton transfer

J. Lahiri, M. Moemeni, J. Kline, I. Magoulas, S. H. Yuwono, M. Laboe, J. Shen, B. Borhan, P. Piecuch, J. E. Jackson et al., The Journal of Chemical Physics 22 (153), 224301 (2020).

Low energy excited state vibrations revealed in conjugated copolymer PCDTBT

S. Irgen‑Gioro, P. Roy, S. Padgaonkar, and E. Harel, The Journal of Chemical Physics 4 (152), 044201 (2020).

Photophysics, morphology and device performances correlation on non-fullerene acceptor based binary and ternary solar cells

G. Zhou, H. Ding, L. Zhu, C. Qiu, M. Zhang, T. Hao, W. Feng, Y. Zhang, H. Zhu, and F. Liu, Journal of Energy Chemistry 47, 180-187 (2020).

Regulating the Packing of Non-Fullerene Acceptors via Multiple Noncovalent Interactions for Enhancing the Performance of Organic Solar Cells

S. Feng, M. Li, N. Tang, X. Wang, H. Huang, G. Ran, Y. Liu, Z. Xie, W. Zhang, and Z. Bo, ACS Applied Materials & Interfaces 4 (12), 4638-4648 (2020).

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ORPHEUS-N Non-Collinear Optical Parametric Amplifier

Product datasheet.

Rev. 18/02/2021. Size 211 KB.

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