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Home > Products > Lasers > Tunable Lasers > Matisse® Tunable Ring Laser

Matisse® Tunable Ring Laser
Matisse® Tunable Ring Laser

  • Fast EOM cavity length stabilization with Pound-Drever-Hall wavelength reference signal assures the narrowest possible spectral linewidth
  • Most efficient ring laser available
  • Wavelength tuning of resonator over 50 GHz with constant output power
  • Dust-sealed housing to avoid optics contamination
  • Massive INVAR baseplate and damping for long-term wavelength stability and low output noise
  • Fast Digital Signal Processing (DSP) with open-source software for convenient and stable laser operation; free software downloads available
  • Sapphire dye jet nozzle for quiet ultra-narrow linewidth output
  • Wavelength meter support with software included
  • All models field-upgradeable

Product Detail Specifications Drawings Downloads
Product Detail

Matisse Family

The Matisse® series is a family of state-of-the-art single frequency ultra-narrow linewidth tunable ring lasers. All Matisse models are built on a mechanically and acoustically isolated massive Invar baseplate for thermal stability and further damping of the individual optical mounts. Each is wavelength-scanned using a precise long-travel piezo to allow single-frequency scanning over 50 GHz while maintaining stable power output without mode hopping. Controlled with high-performance digital signal processing (DSP) technology, Matisse lasers feature user-friendly, open-source software. Taken together, these features provide unprecedented spectral resolution and stability.

With its modular design, the Matisse lasers can be configured – initially at purchase, or later as a field upgrade – for either Ti:Sapphire or a dye solution as the laser gain medium, and for linewidths ranging from 20 MHz down to 30 kHz.

The dye ring laser versions of the Matisse laser are equipped with an innovative high-pressure circulator and sapphire dye jet. The circulators prevent the formation of circulating bubbles and inhibit the transmission of shock waves and vibrations into the liquid jet. This results in a “silent” gain medium that produces the narrowest possible output linewidth with minimum amplitude noise.
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