Coherent mira 900 manual

Mira Optima D. The Mira Optima D incorporates both femtosecond and picosecond cavities in a dual configuration;changing from femto to pico,or vice-versa,is extremely straightforward. Mira S. The Mira S is a standard femtosecond version of the Mira system,withoutthe Optima control package. System expansion for new applications. Coherent Mira Model Laser Operator's Manual Principles of Communications: Systems Modulation and Noise 5ed, Rodger E. Ziemer and William H. Tranter Elements of Optoelectronics and Fiber Optics, Chin-Lin Chen. More Mira oscillators are in use today than any other Kerr lens modelocked Ti:Sapphire laser system. The Mira combines simplicity 1 Specifications apply only with Coherent pump lasers. 2 At nm. 3 For other pump power call factory. 4 Wider coverage possible with short wave or extended long wave optics www.doorway.rug: manual.

More Mira oscillators are in use today than any other Kerr lens modelocked Ti:Sapphire laser system. The Mira combines simplicity and reliability in an innovative design to produce the most powerful and versatile ultrafast laser system available. The innovative design of the Mira system makes switching between. The Mira Family of Ultrafast Ti:sapphire Lasers. The innovative design of the Mira system makes switching between continuous-wave, picosecond and femtosecond operation simple, while passive Kerr lens modelocking provides greater ease-of-use and reliability. Mira OPO-X. Typical Performance Data Figure 1: Any combination of pump and OPO wavelength within these bounded regions is accessible with the Mira OPO-X system. Figure 2: Mira OPO-X (IR) model typical average power. Figure 3: Mira OPO-X (VIS+IR) model typical average power in the visible. OPO Wavelength (nm)

Coherent Laser Group, Coherent Inc., Patrick Henry Drive, 8 8 W to pump the Coherent Mira oscillator and 14 W to. Coherent. Solid-State. Ultrafast. MIRA Modelocked Ti:Sapphire Lasers. Mira Optima F. System Specifications1 Output Power2,3 (Verdi- V5 pump). In a Coherent Mira , pulse energies of more than 50 nJ (at a repetition rate of kHz, and a wavelength of nm) are reached through cavity dumping.