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Soliton-effect compression of supercontinuum to few-cycle durations in photonic nanowires

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Abstract

By exploiting the broad region of anomalous group-velocity dispersion (GVD) and the large effective nonlinearity of photonic nanowires, we demonstrate soliton-effect self-compression of 70-fs pulses down to 6.8 fs. Under suitable conditions, simulations predict that self-compression down to single-cycle duration is possible.

©2005 Optical Society of America

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Supplementary Material (1)

Media 1: AVI (1538 KB)     

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Figures (7)

Fig. 1.
Fig. 1. Group-velocity dispersion of a circular glass nanowire in air for core diameters of 200 nm, 400 nm, 600 nm, and 800 nm.
Fig. 2.
Fig. 2. Group-velocity dispersion of 800-nm and 1-μm diameter glass rods in air appropriate for compression of an 800-nm center wavelength input pulse.
Fig. 3.
Fig. 3. Theoretically predicted (a) temporal and (b) spectral evolution of a 500-pJ and initially 30-fs Gaussian pulse undergoing soliton-effect compression in a 800-nm core diameter photonic nanowire at propagation distances of 501 μm, 582 μm, and 650 μm. (c) Spectrogram representation of the pulse at each of the corresponding propagation distances. (1.54 MB)
Fig. 4.
Fig. 4. Peak intensity of 250-pJ, 375-pJ, 500-pJ, and 750-pJ pulses as a function of propagation distance inside an 800-nm core diameter photonic nanowire.
Fig. 5.
Fig. 5. (a) Optical microscope image of 660-nm and 980-nm core diameter photonic nanowires with 2-mm lengths mounted on a 1-mm metal ridge. (b) Supercontinuum generated in a 2-mm long photonic nanowire.
Fig. 6.
Fig. 6. Measured and simulated spectral evolution of supercontinuum generated as functions of average power of the mode-locked laser before the coupling objective (experiment) and inside the nanowire (simulation).
Fig. 7.
Fig. 7. (a) Measured, retrieved, and simulated XFROG spectrogram of the compressed pulse exiting the nanowire. (b) Retrieved pulse shape and spectrum from the XFROG measurement.

Equations (3)

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z opt L D = 0.32 N + 1.1 N 2 ,
F c = T in T comp ,
Q c = P comp F c ,
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