Grating compensation of third-order material dispersion in the normal dispersion regime: Sub-100-fs chirped-pulse amplification using a fiber stretcher and grating-pair compressor

We describe a method for compensating large amounts of second- and third-order material dispersion, and we present two simple, compact and robust stretcher-compressor systems for microjoule-and millijoule-level chirped-pulse amplification. These systems, which use dispersive material to stretch and a modified grating pair to compress the pulse, provide expansion and compression with full cubic-phase compensation. Unlike previous fiber-stretcher systems which were limited to picosecond pulse durations, these systems can be used effectively with 50-fs microjoule pulses or 100-fs millijoule pulses. The results of our model are described, including the quartic-phase limitations for both systems. We discuss other applications of this grating pair to other areas of ultrafast optics, including intracavity dispersion compensation for femtosecond oscillators. >

[1]  W. White,et al.  Compensation of higher-order frequency-dependent phase terms in chirped-pulse amplification systems. , 1993, Optics letters.

[2]  B. Lemoff,et al.  Cubic-phase-free dispersion compensation in solid-state ultrashort-pulse lasers. , 1993, Optics letters.

[3]  Gerard Mourou,et al.  Generation of ultrahigh peak power pulses by chirped pulse amplification , 1988 .

[4]  P. Becker,et al.  Compression of optical pulses to six femtoseconds by using cubic phase compensation. , 1987, Optics letters.

[5]  H. Haus,et al.  Effect of third-order dispersion on passive mode locking. , 1993, Optics letters.

[6]  W S Colburn,et al.  Chirped-pulse amplification of 85-fs pulses at 250 kHz with third-order dispersion compensation by use of holographic transmission gratings. , 1994, Optics letters.

[7]  B. Lemoff,et al.  Quintic-phase-limited, spatially uniform expansion and recompression of ultrashort optical pulses. , 1993, Optics letters.

[8]  M. Stern,et al.  A simple femtosecond optical third-order disperser , 1991 .

[9]  James P. Gordon,et al.  Negative group-velocity dispersion using refraction , 1984 .

[10]  M. Stern,et al.  Grating compensation of third-order fiber dispersion , 1992 .

[11]  E. Treacy Optical pulse compression with diffraction gratings , 1969 .

[12]  Z. Bor,et al.  Dispersion of optical materials used for picosecond spectroscopy. , 1985, Applied optics.

[13]  G. Mourou,et al.  Chirped-pulse amplification of 100-fsec pulses. , 1989, Optics letters.

[14]  P. Tournois,et al.  Theory of a New Parallel Diffraction Grating Delay Line for Linear FM Pulse Compression , 1971, IEEE Transactions on Sonics and Ultrasonics.

[15]  Oscar E. Martínez,et al.  3000 times grating compressor with positive group velocity dispersion: Application to fiber compensation in 1.3-1.6 µm region , 1987 .

[16]  P. Tournois New diffraction grating pair with very linear dispersion for laser pulse compression , 1993 .