Skip to main content
White Dwarf HE tunable high enery lasers for scientific applications
beamline lasers
  • White Dwarf HE tunable high enery lasers for scientific applications
  • beamline lasers

White Dwarf HE – tunable high enery lasers for scientific applications

Few-cycle OPCPA for fundamental research
  • high average power up to 30 W
  • few-cycle pulse durations below 10 fs
  • wavelength versions from 800 nm up to 9 µm
  • optional CEP stability
  • pumped by industry-grade Yb-amplifiers with up to 300 W and 3 mJ
Request a quote
Details
Request a quote

Introduction

Features

High average power

up to 30 W average power at high repetition rates

Passive CEP stability

Intrinsic carrier-envelope-stability for highest-precision attosecond science

Wavelength from UV to mid-IR

Systems available from 200 – 10.000 nm

Robustness and compactness

Industrial grade pump lasers based on Yb-technology

Specs

WD-HE-Attodriver WD-HE-800 WD-HE-1500 WD-HE-2000 WD-HE-3000 WD-HE-MIR
Central wavelength 800 nm 800 nm 1500 nm 2000 nm 3000 nm 9000
Pulse duration FWHM < 10 fs < 10 fs < 40 fs < 40 fs < 80 fs < 120 fs
Average power 6 W 25 W 35 W 25 W 15 W 3 W
Pulse energy compressed  up to 150 µJ 250 µJ 350 µJ 250 µJ 150 µJ 1.2 µJ
Repetition rate 40 – 200 kHz 100 kHz 100 kHz 100 kHz 100 kHz 0.1 – 1 MHz
Beam quality M2 < 1.3 < 1.3 < 1.5 < 1.5 < 1.5 < 1.5
Power stability 12 hrs < 1% < 1% < 1.5 % < 1.5 % < 1.5 % < 1.5 %
Dimensions (OPCPA) 80 cm x 120 cm 80 cm x 120 cm 80 cm x 120 cm 80 cm x 120 cm 80 cm x 120 cm 80 cm x 120 cm
Pump laser incl. 80 W* 300 W 300 W 300 W 300 W 300 W

*integrated in OPCPA-box

Performance

Applications

Downloads

FAQ

Publications

  • February 1, 2021
    Optical properties of Li-based nonlinear crystals for high power mid-IR OPCPA pumped at 1 µm under realistic operational conditions,” Opt. Mater. Express 11, 231-239 (2021)
    https://doi.org/10.1364/OME.414478
  • May 10, 2019
    A high power (11 W), tunable (1.45–1.65 µm) OPCPA for THz generation in organic crystals, in Conference on Lasers and Electro-Optics, OSA Technical Digest (Optical Society of America, 2019), paper STh3E.3.
    https://doi.org/10.1364/CLEO_SI.2019.STh3E.3
  • March 2, 2020
    Dual channel laser system with gap-less tuning from 250-1300 nm at megahertz repetition rates for time-resolved photoelectron-emission microscopy and spectroscopy,” Proc. SPIE 11264, Nonlinear Frequency Generation and Conversion: Materials and Devices XIX, 1126415
    https://doi.org/10.1117/12.2546247
  • May 15, 2020
    Dual-channel laser system with gap-less tuning from 250 – 1300 nm at megahertz repetition rates for time-resolved photoelectron-emission microscopy and spectroscopy, Conference on Lasers and Electro-Optics, OSA Technical Digest (Optical Society of America, 2020), paper JW2F.22.
    https://doi.org/10.1364/CLEO_AT.2020.JW2F.22
  • March 5, 2021
    High power 9 μm source for spectroscopy and HHG, Proc. SPIE 11670, Nonlinear Frequency Generation and Conversion: Materials and Devices XX; 116700X (2021)
    https://doi.org/10.1117/12.2576133
  • February 21, 2020
    High power CEP-stable OPCPA at 800nm,” Proc. SPIE 11259, Solid State Lasers XXIX: Technology and Devices, 112591L
    https://doi.org/10.1117/12.2546254
  • April 5, 2022
    Prakriti P. Joshi, Ruiyu Li, … and Sarah B. King, Nanoimaging of the Edge-Dependent Optical Polarization Anisotropy of Black Phosphorus, Nano Lett. 2022, 22, 8, 3180–3186
    https://doi.org/10.1021/acs.nanolett.1c03849
  • October 19, 2023
    Chlouba, T., Shiloh, R., Kraus, S. et al. Coherent nanophotonic electron accelerator. Nature 622, 476–480 (2023)
    https://doi.org/10.1038/s41586-023-06602-7

Related Products