We present simulations for a design of a high-energy single-stage mid-IR difference frequency generation adapted to a two-color Ti:sapphire amplifier system. The optimized mixing process is based on chirped pulse difference frequency generation (CP-DFG), allowing for a higher conversion efficiency and reduced two-photon absorption losses. The numerical start-to-end simulations include stretching, chirped pulse difference frequency generation and pulse compression. Realistic design parameters for commercially available nonlinear crystals (GaSe, AgGaS2, LiInSe2, LiGaSe2) are considered. Compared with conventional unchirped DFG directly pumped by Ti:sapphire technology, we predict a threefold increase in the quantum efficiency. Our CP-DFG sche...
In this thesis, I have developed a tunable two-color two-stage ultrafast Yb:fiber chirped pulse ampl...
One of the exciting advances in ultra-fast optics is the development of a new amplifier architecture...
A number of manners to obtain first-order achromatic phase matching of both type I and type II are p...
A design for efficient generation of mid-infrared pulses at 3.2 μm is presented, which is based on n...
Few-cycle carrier-envelope phase (CEP) stable laser pulses enable the precise control of strong-fiel...
Stable subpicosecond infrared pulses in the spectral region of 4.5-11.5 ,um are generated by differe...
Generating the difference frequency of a frequency-doubled, widely tunable Ti:Al2O3 laser and a Nd:Y...
The maximum energy achievable directly from conventional Ti:sapphire oscillators has been limited by...
Frequency combs in the mid-IR wavelength are usually implemented by difference-frequency generation ...
Abstract. : We demonstrate a novel scalable and engineerable approach for the frequency-doubling of ...
We demonstrate generation of two synchronized picosecond pulses at different wavelengths near 778 nm...
We employ AgGaSe(2) for difference-frequency generation between signal and idler of synchronously-pu...
By employing a dual-chirped optical parametric amplification (DC-OPA) using MgO:LiNbO3 crystals, we ...
A powerful mid-infrared frequency comb in the 2-20 μm range plays a very important role in the deve...
The mid-infrared (MIR) system presented in the thesis is based on a sub-100-fs erbium-doped fiber la...
In this thesis, I have developed a tunable two-color two-stage ultrafast Yb:fiber chirped pulse ampl...
One of the exciting advances in ultra-fast optics is the development of a new amplifier architecture...
A number of manners to obtain first-order achromatic phase matching of both type I and type II are p...
A design for efficient generation of mid-infrared pulses at 3.2 μm is presented, which is based on n...
Few-cycle carrier-envelope phase (CEP) stable laser pulses enable the precise control of strong-fiel...
Stable subpicosecond infrared pulses in the spectral region of 4.5-11.5 ,um are generated by differe...
Generating the difference frequency of a frequency-doubled, widely tunable Ti:Al2O3 laser and a Nd:Y...
The maximum energy achievable directly from conventional Ti:sapphire oscillators has been limited by...
Frequency combs in the mid-IR wavelength are usually implemented by difference-frequency generation ...
Abstract. : We demonstrate a novel scalable and engineerable approach for the frequency-doubling of ...
We demonstrate generation of two synchronized picosecond pulses at different wavelengths near 778 nm...
We employ AgGaSe(2) for difference-frequency generation between signal and idler of synchronously-pu...
By employing a dual-chirped optical parametric amplification (DC-OPA) using MgO:LiNbO3 crystals, we ...
A powerful mid-infrared frequency comb in the 2-20 μm range plays a very important role in the deve...
The mid-infrared (MIR) system presented in the thesis is based on a sub-100-fs erbium-doped fiber la...
In this thesis, I have developed a tunable two-color two-stage ultrafast Yb:fiber chirped pulse ampl...
One of the exciting advances in ultra-fast optics is the development of a new amplifier architecture...
A number of manners to obtain first-order achromatic phase matching of both type I and type II are p...