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The \"DCM9\" is a GVD mirror shifted to the \"blue\" now covering a wavelength range of 450nm-950nm. These mirrors are specially designed to be suitable for pulse compression of femtosecond pulses generated by amplification, filamentation, OPA/OPG and others. Featuring negative GVD of -60 fs² for the mirror pair @ 700nm and are ...
  • Wavelength Range: 450 - 950 nm
  • Reflectivity: 99.6 %
  • GDD/pair: 60 fs^2
  • Angle Of Incidence: 0 - 10 Degrees
  • Substrate: Fused Silica
Data Sheet
The \"DCM7\" is a ultra-broadband (600nm-1200nm) dispersion compensating mirror pair used for the compensation of positive dispersion affecting femtosecond laser pulses. The unique pair design enables to achieve a reflectivity greater than 99.9% over the whole supported spectral bandwidth next to a defined negative dispersion. These ...
  • Wavelength Range: 600 - 1200 nm
  • Reflectivity: 99.6 %
  • GDD/pair: 120 fs^2
  • Angle Of Incidence: 0 - 10 Degrees
  • Substrate: Fused Silica
Data Sheet
The \"DCM11\" is a GVD mirror pair specially designed for OPCPA compression. This mirror type covers a wide wavelength range of 650-1050 nm while offering a large dispersion of -130 fs2 /pair at the centre wavelength of 800 nm. These mirrors are specially designed to recompress the output of the venteon OPCPA after passing through ...
  • Wavelength Range: 650 - 1050 nm
  • Reflectivity: 99.8 %
  • GDD/pair: 130 fs^2
  • Angle Of Incidence: 0 - 10 Degrees
  • Substrate: Fused Silica
Data Sheet
The \"DCM10\" is a broadband (500-850nm) dispersion compensating mirror pair designed for the compensation of the positive dispersion caused by fused silica like material. The wavelength range suits femtosecond applications using few-cycle pulses generated by hollow core fibers or filamentation. The unique pair design enables to ...
  • Wavelength Range: 500 - 850 nm
  • Reflectivity: 99.6 %
  • GDD/pair: 100 fs^2
  • Angle Of Incidence: 0 - 10 Degrees
  • Substrate: UV Grade Fused Silica
Data Sheet

Did You know?

Chirped dielectric laser mirrors offer a general solution for broadband feedback and dispersion control in femtosecond laser systems. Chirped mirrors were developed for mode-locked solid-state lasers, femtosecond parametric oscillators, chirped pulse amplification systems and pulse compressors for dispersive compensation and to get a broader reflection bandwidth. The principle of operation of these mirrors is that different wavelengths penetrate the layers of the mirror coating to various depths thus creating dispersion (delay) within the spectrum of wavelengths. A double chirped design has been also devised which turns on the coupling between counter propagating waves and removes Fresnel reflection with an application of anti-reflection film. Double-chirped mirror designs can also be utilized with semiconductor mirrors to generate much higher amount of dispersion.