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Laboratory for X-Ray Microimaging and Bioinformatics
 

Oscillator


We have combined techniques to generate the high-energy laser, then converted the wavelength to ultraviolet by third harmonic generation, and finally amplified to the terawatt order output through the KrF* excimer amplifier.
Our facility is capable of producing ~400 mJ, 230 fs, 248 nm with near diffraction limited beam quality at a 0.4 Hz reparation rate.
 
 
Ti:Sapphire oscillator laser system
 

 
Our Ti:Sapphire femtosecond oscillator was developed using self-mode-locked principle. The cavity configuration is shown in the block schematic diagram. This cavity consistes of an end mirror, an output coupler, a pair of prisms, focusing fold mirrors, birefringent filter, tuning slit, and Ti:Sapphire crystal. A 6.7 W of all-link radiation from a Coherent Innova 300 Ar-ion laser is focused into the Ti:Sapphire crystal, collinear with the mode of the cavity itself. The Ti:Sapphire crystal rod is Brewster-angle cut, 1.0 cm in length. Two concave mirrors in an off-axis "Z" configuration allow the compensation of astigmatism, while a pair of Brewster-cut fused silica (SF11) prisms are used to compensate for spectral dispersion (chirp) of the crystal. A single-plate birefringent filter ins inserted in the cavity to choose the central wavelength over the range 720-850 nm. Pulsing is established by tapping of the prism pair femtosecond laser and chirped pulse amplification (CPA).
 
 

 
Fig.2: Diagram of Ti:Sapphire self-mode-locked oscillator and pulse stretcher
 

 
 
 
References:
 
 
1. D.E. Spence, P.N. Kean, and W. Sibbet, Opt. Lett. 16, 42 (1991).
 
 
 
 
 
 
 
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