Dispersion considerations in ultrafast CPA systems

A basic assumption underlies many designs for chirped-pulse amplification (CPA) of ultrashort pulses. This assumption is that a Taylor's series expansion of the dispersive delay is well behaved in the sense that each phase order in the expansion produces an effect on the pulse that is significantly smaller than the effect of the previous order. This work investigates this assumption both qualitatively and quantitatively. We show quantitatively that the requirements for achieving sub-20-fs pulses are much more stringent than for 100-fs pulses. We find that when the basic assumption holds, a chirped pulse amplification (CPA) system may be designed by zeroing each order in succession, but that zeroing may not work well for some systems that are not well behaved. For these cases minimizing the overall dispersion becomes necessary. We discuss some common optical components including bulk materials, expanders, and compressors and show that they generally satisfy the basic assumption. Finally, we discuss the problem of optimizing a CPA system in the laboratory, and describe a new polarization-gate (PC) frequency-resolved optical gating (FROG) arrangement that is based on thin-film polarizers and that allows accurate measurements of the phase as well as the intensity with minimal dispersive effects.

[1]  C. Froehly,et al.  Autocorrelation of laser pulses by optical processing of Fabry-Perot spectrograms. , 1980, Applied optics.

[2]  P. Yeh Autocorrelation of ultrashort optical pulses using polarization interferometry. , 1983, Optics letters.

[3]  R. Trebino,et al.  Phase and intensity characterization of femtosecond pulses from a chirped-pulse amplifier by frequency-resolved optical gating. , 1995, Optics letters.

[4]  D. Kane,et al.  Using phase retrieval to measure the intensity and phase of ultrashort pulses: frequency-resolved optical gating , 1993 .

[5]  M. Joffre,et al.  Two-dimensional nonlinear optics using Fourier-transform spectral interferometry. , 1996, Optics letters.

[6]  A. Alcock,et al.  Ultraviolet and visible single‐shot autocorrelator based on multiphoton ionization , 1986 .

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

[8]  P. Georges,et al.  Single-shot measurement of a 52-fs pulse. , 1987, Applied optics.

[9]  T. Yajima,et al.  A rapid scanning interferometric autocorrelator for monitoring femtosecond pulses , 1989 .

[10]  M M Murnane,et al.  Amplification of 26-fs, 2-TW pulses near the gain-narrowing limit in Ti:sapphire. , 1995, Optics letters.

[11]  J G Fujimoto,et al.  Measurement of the amplitude and phase of ultrashort light pulses from spectrally resolved autocorrelation. , 1993, Optics letters.

[12]  K R Wilson,et al.  Generation of 18-fs, multiterawatt pulses by regenerative pulse shaping and chirped-pulse amplification. , 1996, Optics letters.

[13]  Gregory E. Hall,et al.  CW autocorrelation measurements of picosecond laser pulses , 1980 .

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

[15]  S. Saltiel,et al.  A diffraction grating autocorrelator for measurement of single ultrashort light pulses , 1984 .

[16]  K R Wilson,et al.  Regenerative pulse shaping and amplification of ultrabroadband optical pulses. , 1996, Optics letters.

[17]  N. Blanchot,et al.  Amplification of sub-100-TW femtosecond pulses by shifted amplifying Nd:glass amplifiers: theory and experiments. , 1995, Optics letters.

[18]  Gerard Mourou,et al.  Compression of amplified chirped optical pulses , 1985 .

[19]  Jeffrey A. Squier,et al.  Grism-pair stretcher–compressor system for simultaneous second- and third-order dispersion compensation in chirped-pulse amplification , 1997 .

[20]  Victor Wong,et al.  Ultrashort-pulse characterization from dynamic spectrograms by iterative phase retrieval , 1997 .

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

[22]  J P Heritage,et al.  Direct measurement of the spectral phase of femtosecond pulses. , 1995, Optics letters.

[23]  W. White,et al.  Phase control for production of high-fidelity optical pulses for chirped-pulse amplification. , 1995, Optics letters.

[24]  C. Barty,et al.  Generation of 16-fs, 10-TW pulses at a 10-Hz repetition rate with efficient Ti:sapphire amplifiers. , 1998, Optics letters.

[25]  B. Lemoff,et al.  Multiterawatt 30-fs Ti:sapphire laser system. , 1994, Optics letters.

[26]  S. Kane,et al.  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 , 1995 .

[27]  G. Mourou,et al.  Terawatt to Petawatt Subpicosecond Lasers , 1994, Science.

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

[29]  G Tietbohl,et al.  125-TW Ti:sapphire/Nd:glass laser system. , 1997, Optics letters.

[30]  D N Fittinghoff,et al.  Transient-grating frequency-resolved optical gating. , 1997, Optics letters.

[31]  F. Kärtner,et al.  Self-starting 6.5-fs pulses from a Ti:sapphire laser. , 1997, Optics letters.

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

[33]  D N Fittinghoff,et al.  Measurement of the intensity and phase of ultraweak, ultrashort laser pulses. , 1996, Optics letters.

[34]  O. Martínez,et al.  Direct determination of the amplitude and the phase of femtosecond light pulses. , 1991, Optics letters.

[35]  Rick Trebino,et al.  Comparison of ultrashort-pulse frequency-resolved-optical-gating traces for three common beam geometries , 1994 .

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

[37]  D N Fittinghoff,et al.  Frequency-resolved optical-gating measurements of ultrashort pulses using surface third-harmonic generation. , 1996, Optics letters.

[38]  G. Grillon,et al.  Third order autocorrelation study of amplified subpicosecond laser pulses , 1983 .

[39]  I. Christov,et al.  Measurement of 10-fs laser pulses , 1996 .

[40]  E. Kintzer,et al.  Near-surface second-harmonic generation for autocorrelation measurements in the uv , 1987 .

[41]  B. Sugg,et al.  Refractive Index of Terbium Gallium Garnet , 1994 .

[42]  W. White,et al.  Recent developments in the measurement of the intensity and phase of ultrashort pulses using frequency-resolved optical gating , 1994, Proceedings of 1994 Nonlinear Optics: Materials, Fundamentals and Applications.

[43]  A. Tünnermann,et al.  Single-shot autocorrelator for KrF subpicosecond pulses based on two-photon fluorescence of cadmium vapor at lambda = 508 nm. , 1991, Optics letters.

[44]  D. Kane,et al.  Single-shot measurement of the intensity and phase of an arbitrary ultrashort pulse by using frequency-resolved optical gating. , 1993, Optics letters.

[45]  Oscar E. Martínez,et al.  Design of high-power ultrashort pulse amplifiers by expansion and recompression , 1987 .

[46]  Mark Beck,et al.  Group delay measurements of optical components near 800 nm , 1991 .

[47]  Z Bor,et al.  Phase-sensitive single-pulse autocorrelator for ultrashort laser pulses. , 1988, Optics letters.

[48]  X. Steve Yao,et al.  Measuring the coherence length of mode‐locked laser pulses in real time , 1990 .