Suppression of the pedestal in a chirped-pulse-amplification laser

The pedestal (prepulse and postpulse) associated with a chirped-pulse-amplification (CPA) laser is studied. Four components have been identified that contribute to the pedestal. Pulses are spectrally shaped by gain narrowing in a frequency-matched, regenerative amplifier, while self-phase modulation is avoided. The intensity contrast is further improved through the use of a saturable absorber, resulting in Gaussian pulses of ~0.9-ps duration with an intensity contrast exceeding 105:1. Both experimental and numerical descriptions of these processes are presented. This investigation makes possible the study of high-intensity ultrashort laser–plasma interactions with a fiber–grating CPA system.

[1]  Wolfgang Zinth,et al.  Generation of chirp-free picosecond pulses , 1977 .

[2]  Compensation of nonlinear chirp generated by self-steepening using third order dispersion of a grating pair , 1988 .

[3]  M. Perry,et al.  Spectral shaping in chirped-pulse amplification. , 1990, Optics letters.

[4]  J. McMullen,et al.  Analysis of compression of frequency chirped optical pulses by a strongly dispersive grating pair. , 1979, Applied optics.

[5]  Justin Peatross,et al.  Modeling the pedestal in a chirped-pulse-amplification laser , 1991, Photonics West - Lasers and Applications in Science and Engineering.

[6]  W. J. Tomlinson Curious features of nonlinear pulse propagation in single-mode optical fibers , 1989 .

[7]  Delamater,et al.  Kilovolt x-ray spectroscopy of a subpicosecond-laser-excited source. , 1989, Physical review. A, General physics.

[8]  Oscar E. Martínez,et al.  Grating and prism compressors in the case of finite beam size , 1986 .

[9]  Falcone,et al.  High density plasmas produced by ultrafast laser pulses. , 1989, Physical review letters.

[10]  Andrew M. Weiner,et al.  Spectral windowing of frequency‐modulated optical pulses in a grating compressor , 1985 .

[11]  Michael D. Perry,et al.  X-ray characterization of picosecond laser plasmas☆ , 1987 .

[12]  J. Harvey,et al.  Efficient high-power optical pulse compression with logarithmic wing analysis , 1987 .

[13]  K. Drexhage,et al.  New ultrafast saturable absorbers for Nd: Lasers , 1980 .

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

[15]  D. Grischkowsky,et al.  Optical pulse reshaping based on the nonlinear birefringence of single-mode optical fibers. , 1983, Optics letters.

[16]  G. Mourou,et al.  Temporal shape analysis of Nd/3+/:YAG active passive mode-locked pulses , 1981 .

[17]  Andrew M. Weiner,et al.  Stabilized pulse compression by multiple-order stimulated Raman scattering with group velocity dispersion , 1988 .

[18]  Gerard Mourou,et al.  1000 times expansion/compression of optical pulses for chirped pulse amplification , 1987 .

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

[20]  Philippe Bado,et al.  Regenerative amplification of picosecond pulses in Nd:YLF: gain narrowing and gain saturation , 1988 .

[21]  D. Grischkowsky,et al.  Simultaneous optical pulse compression and wing reduction , 1986, Annual Meeting Optical Society of America.

[22]  Y. Kato,et al.  Generation of a high-energy picosecond laser pulse with a high-contrast ratio by chirped-pulse amplification , 1991 .

[23]  R. Stolen,et al.  Intensity discrimination of optical pulses with birefringent fibers. , 1982, Optics letters.