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High energy femtosecond Yb cubicon fiber amplifier

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Abstract

The generation of cubicon pulses from an Yb fiber chirped pulse amplification system at pulse energies up to 200 µJ is demonstrated. After pulse compression 650 fs pulses with a pulse energy of 100 µJ are obtained, where pulse compression relies on the compensation of third-order dispersion mismatch between the stretcher and compressor via self-phase modulation of the cubicon pulses in the fiber amplifier. Values of self-phase modulation well in excess of π can be tolerated for cubicon pulses, allowing for the nonlinear compensation of very large levels of dispersion mismatch between pulse stretcher and compressor.

©2005 Optical Society of America

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Figures (6)

Fig. 1.
Fig. 1. Yb fiber amplifier chain for generation of high energy femtosecond pulses.
Fig. 2.
Fig. 2. Autocorrelations of compressed cubicon pulses at 10 µJ (left) and 50 µJ (right).
Fig. 3.
Fig. 3. Cubicon pulse spectra at 10 µJ (left) and 50 µJ (right).
Fig. 4.
Fig. 4. Cross-correlation between fundamental and frequency-doubled cubicon pulses for 10 µJ (dashed) and 50 µJ (solid) plotted on linear (left) and logarithmic (right) scales
Fig. 5.
Fig. 5. Theoretical cross-correlation (left) between fundamental and frequency-doubled cubicon pulses for 10 µJ (dashed) and 50 µJ (solid) plotted on a logarithmic scale. Corresponding pulse spectrum for 50 µJ (right).
Fig. 6.
Fig. 6. Autocorrelations of compressed cubicon pulses at 10 µJ (left) and 100 µJ (right), illustrating pulse cleaning with increasing pulse energy

Equations (1)

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A z = i γ A 2 A i 2 β 2 2 A t 2 + 1 6 β 3 3 A t 3 + g ( ω , z ) A
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