System and method for high-intensity ultrashort pulse compression
A system comprising a laser emitting an ultrashort pulse beam; and a dielectric bulk medium having a refractive index depending on intensity, the bulk medium broadening the laser beam homogeneously versus transversal spatial coordinates, and a method for compressing high energy femtosecond laser pulses, comprising propagating the laser beam inside a dielectric bulk medium having a refractive index depending on the beam intensity, the bulk medium broadening the laser beam homogeneously versus transversal spatial coordinates; and compressing a resulting broadened spectrum.
1. A system, comprising:
a laser emitting an ultrashort pulse beam; and
a dielectric bulk medium having a refractive index depending on intensity, said bulk medium broadening the laser beam homogeneously;
wherein said bulk medium has a varying thickness such that a product of a thickness of the bulk medium by the laser beam intensity is constant across the beam.
2. The system of claim 1 , wherein said bulk medium is selected to be transparent to propagated and generated wavelengths.
3. The system of claim 1 , further comprising a conjugated optics collimating the laser beam after its propagation through the bulk medium.
4. The system of claim 3 , further comprising chirped mirrors to compress the broadened spectrum to a shorter pulse.
5. The system of claim 3 , further comprising a medium delaying longer wavelengths of the broadened spectrum.
6. The system of claim 1 , installed inside a vacuum chamber.
7. The system of claim 1 , kept in an inert gas environment.
8. The system of claim 1 , wherein said laser is one of: a terawatt and above femto second laser.
9. A system, comprising:
a laser emitting an ultrashort pulse beam; and
a dielectric bulk medium having a refractive index depending on intensity, said bulk medium broadening the laser beam homogeneously;
wherein the beam of said laser has a Gaussian profile and said bulk medium is a lens having a varying thickness selected so that it has, at a radial position corresponding to 1/e of the beam energy, a thickness e times higher than a thickness at a central part of the lens, e being the Euler's number.
10. The system of claim 9 , further comprising an off-axis parabola placed after said lens.