Fig. 1. Schematic diagram of two-pass two-grating compressor

Fig. 2. Schematic of aperture function of different frequencies light on the plane of lens. (a) ω<ω0; (b) ω>ω0

Fig. 3. Optical phase distribution of input pulse and far-field spatial-temporal distribution of output pulse. (a) Ideal plane wavefront; (b) ideal far-field spatial-temporal distribution; (c) random wavefront distortion; (d) far-field spatial-temporal distribution of wavefront distortion as shown in Fig. 3(c)

Fig. 4. Relationship between the wavefront distortion of input laser pulse and SR of compressor

Fig. 5. Influences of grating diffraction plane deformation on output pulse. (a) Deformation of grating diffraction plane; (b) far-field spatial-temporal distribution; (c) time distribution of the dotted line of Fig.5(b)

Fig. 6. (a) Spectral phase changes versus spatial position across the grating groove direction for different frequencies light caused by grating deformation; (b) group delay across the grating groove direction; (c) relationship between the PV of grating deformation and the output performance of compressor

Fig. 7. Wave aberrations and far-field spatial-temporal distributions of pulse. (a) Spherical; (b) far-field spatial-temporal distribution of spherical; (c) coma; (d) far-field spatial-temporal distribution of coma; (e) astigmatism; (f) far-field spatial-temporal distribution of astigmatism

Fig. 8. Spectral phase changes versus spatial position across the grating groove direction for different frequencies light caused by wave aberrations. (a) Spherical; (b) coma; (c) astigmatism; (d) group delay across the grating groove direction caused by wave aberrations

Fig. 9. Relationships between the wave aberrations of grating and the property of compressor output. (a) Spherical; (b) coma; (c) astigmatism