Pulse front and pulse duration distortion in refractive optics, and its compensation
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[1] T. Elsaesser,et al. Picosecond dye laser emission in the infrared between 1.4 and 1.8 μm , 1983 .
[2] Bela Racz,et al. Group velocity dispersion in prisms and its application to pulse compression and travelling-wave excitation , 1985 .
[3] James P. Gordon,et al. Negative group-velocity dispersion using refraction , 1984 .
[4] I. McIntyre,et al. Subpicosecond KrF* excimer-laser source. , 1986, Optics letters.
[5] Z. Bor,et al. Dispersion of optical materials used for picosecond spectroscopy. , 1985, Applied optics.
[6] Michael R. Topp,et al. Group dispersion effects in picosecond spectroscopy , 1975 .
[7] F. Schäfer,et al. Bandwidth limited amplification of 220 fs pulses in XeCl , 1987 .
[8] R. Wyatt,et al. Versatile single-shot background-free pulse duration measurement technique, for pulses of subnanosecond to picosecond duration , 1981 .
[9] P. Laporta,et al. The role of cavity dispersion in CW mode-locked dye lasers , 1984 .
[10] Sándor Szatmári,et al. Simplified laser system for the generation of 60 fs pulses at 248 nm , 1988 .
[11] J. Misewich,et al. Ultrafast ultraviolet pump–probe apparatus , 1986 .
[12] F. Schäfer,et al. Hybrid dye-excimer laser system for the generation of 80 fs, 900 GW pulses at 248 nm , 1987 .
[13] E. Treacy. Optical pulse compression with diffraction gratings , 1969 .
[14] M. R. Topp. Oscilloscope display of picosecond fluctuations in light intensity , 1975 .
[15] A. Müller,et al. Picosecond pulse shortening by travelling wave amplified spontaneous emission , 1983 .